Ethylene Basics

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c 2005 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim 10.1002/14356007.a10 045 Ethylene 1 Ethylene Heinz Zimmermann, Linde AG, Hoellriegelskreuth, Federal Republic of Germany Roland Walzl, Linde AG, Hoellriegelskreuth, Federal Republic of Germany 1. Introduction .............. 1 2. Physical Properties .......... 2 3. Chemical Properties ......... 2 4. Raw Materials ............. 3 5. Production ............... 4 5.1. Ethylene from Pyrolysis of Hydro- carbons ................. 4 5.1.1. Cracking Conditions ......... 4 5.1.2. Heat Requirements for Hydrocarbon Pyrolysis ................. 9 5.1.3. Commercial Cracking Yields .... 10 5.1.4. Commercial Cracking Furnaces .. 15 5.1.5. Tube Metallurgy ............ 23 5.1.6. Thermal Efficiency of Ethylene Fur- naces ................... 23 5.1.7. Coking and Decoking of Furnaces and Quench Coolers .......... 25 5.2. Quenching of Hot Cracked Gas . 26 5.3. Recovery Section ........... 31 5.3.1. Products ................. 32 5.3.2. Cracked Gas Processing ....... 33 5.3.2.1. Front-End Section ........... 33 5.3.2.2. Hydrocarbon Fractionation Section 36 5.3.3. Utilities ................. 44 5.3.4. Process Advances ........... 45 5.4. Other Processes and Feedstocks . 46 6. Environmental Protection ..... 47 7. Quality Specifications ........ 48 8. Chemical Analysis .......... 48 9. Storage and Transportation .... 48 10. Uses and Economic Aspects .... 50 11. Toxicology and Occupational Health .................. 51 12. References ............... 51 1. Introduction Ethylene [74-85-1], ethene, H 2 C=CH 2 , M r 28.52, is the largest-volume petrochemical pro- duced worldwide. Ethylene, however, has no di- rect end uses, being used almost exclusively as a chemical building block. It has been recovered from coke-oven gas and other sources in Europe since 1930 [1]. Ethylene emerged as a large- volume intermediate in the 1940s when U.S. oil and chemical companies began separating it from refinery waste gas and producing it from ethane obtained from refinery byproduct streams and from natural gas. Since then, ethylene has almost completely replaced acetylene for many syntheses. Ethylene is produced mainly by ther- mal cracking of hydrocarbons in the presence of steam, and by recovery from refinery cracked gas. In 1996 total worldwide ethylene production capacity was 79.3 × 10 6 t, with an actual de- mand of ca. 71 × 10 6 t/a [2], which has growth projections of 4.5 % per year worldwide for the period of 1996 to 2005 [3–5]. 2. Physical Properties Ethylene is a colorless flammable gas with a sweet odor. The physical properties of ethylene are as follows: mp 169.15 C bp 103.71 C Critical temperature, T c 9.90 C Critical pressure, Pc 5.117 MPa Critical density 0.21 g/cm 3 Density at bp 0.57 g/cm 3 at 0 C 0.34 g/cm 3 Gas density at STP 1.2603 g/L Density relative to air 0.9686 Molar volume at STP 22.258 L Surface tension at bp 16.5 mN/m at 0 C 1.1 mN/m Heat of fusion 119.5 kJ/kg Heat of combustion 47.183 MJ/kg Heat of vaporization at bp 488 kJ/kg at 0 C 191 kJ/kg Specific heat of liquid at bp 2.63 kJ kg 1 K 1 of gas at T c 1.55 kJ kg 1 K 1 Enthalpy of formation 52.32 kJ/mol

description

Brief description for Ethylene manufacturing

Transcript of Ethylene Basics

Page 1: Ethylene Basics

c© 2005 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim10.1002/14356007.a10 045

Ethylene 1

Ethylene

Heinz Zimmermann, Linde AG, Hoellriegelskreuth, Federal Republic of Germany

Roland Walzl, Linde AG, Hoellriegelskreuth, Federal Republic of Germany

1. Introduction . . . . . . . . . . . . . . 12. Physical Properties . . . . . . . . . . 23. Chemical Properties . . . . . . . . . 24. Raw Materials . . . . . . . . . . . . . 35. Production . . . . . . . . . . . . . . . 45.1. Ethylene from Pyrolysis of Hydro-

carbons . . . . . . . . . . . . . . . . . 45.1.1. Cracking Conditions . . . . . . . . . 45.1.2. Heat Requirements for Hydrocarbon

Pyrolysis . . . . . . . . . . . . . . . . . 95.1.3. Commercial Cracking Yields . . . . 105.1.4. Commercial Cracking Furnaces . . 155.1.5. Tube Metallurgy . . . . . . . . . . . . 235.1.6. Thermal Efficiency of Ethylene Fur-

naces . . . . . . . . . . . . . . . . . . . 235.1.7. Coking and Decoking of Furnaces

and Quench Coolers . . . . . . . . . . 25

5.2. Quenching of Hot Cracked Gas . 265.3. Recovery Section . . . . . . . . . . . 315.3.1. Products . . . . . . . . . . . . . . . . . 325.3.2. Cracked Gas Processing . . . . . . . 335.3.2.1. Front-End Section . . . . . . . . . . . 335.3.2.2. Hydrocarbon Fractionation Section 365.3.3. Utilities . . . . . . . . . . . . . . . . . 445.3.4. Process Advances . . . . . . . . . . . 455.4. Other Processes and Feedstocks . 466. Environmental Protection . . . . . 477. Quality Specifications . . . . . . . . 488. Chemical Analysis . . . . . . . . . . 489. Storage and Transportation . . . . 4810. Uses and Economic Aspects . . . . 5011. Toxicology and Occupational

Health . . . . . . . . . . . . . . . . . . 5112. References . . . . . . . . . . . . . . . 51

1. Introduction

Ethylene [74-85-1], ethene, H2C=CH2, Mr28.52, is the largest-volume petrochemical pro-duced worldwide. Ethylene, however, has no di-rect end uses, being used almost exclusively asa chemical building block. It has been recoveredfrom coke-oven gas and other sources in Europesince 1930 [1]. Ethylene emerged as a large-volume intermediate in the 1940s when U.S.oil and chemical companies began separating itfrom refinery waste gas and producing it fromethane obtained from refinery byproduct streamsand from natural gas. Since then, ethylene hasalmost completely replaced acetylene for manysyntheses. Ethylene is produced mainly by ther-mal cracking of hydrocarbons in the presenceof steam, and by recovery from refinery crackedgas.

In 1996 total worldwide ethylene productioncapacity was 79.3× 106 t, with an actual de-mand of ca. 71× 106 t/a [2], which has growthprojections of 4.5 % per year worldwide for theperiod of 1996 to 2005 [3–5].

2. Physical Properties

Ethylene is a colorless flammable gas with asweet odor. The physical properties of ethyleneare as follows:

mp −169.15 ◦Cbp −103.71 ◦CCritical temperature, Tc 9.90 ◦CCritical pressure, Pc 5.117MPaCritical density 0.21 g/cm3

Densityat bp 0.57 g/cm3

at 0 ◦C 0.34 g/cm3

Gas density at STP 1.2603 g/LDensity relative to air 0.9686Molar volume at STP 22.258 LSurface tensionat bp 16.5mN/mat 0 ◦C 1.1mN/m

Heat of fusion 119.5 kJ/kgHeat of combustion 47.183MJ/kgHeat of vaporizationat bp 488 kJ/kgat 0 ◦C 191 kJ/kg

Specific heatof liquid at bp 2.63 kJ kg−1 K−1

of gas at Tc 1.55 kJ kg−1 K−1

Enthalpy of formation 52.32 kJ/mol

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Entropy 0.220 kJmol−1 K−1

Thermal conductivityat 0 ◦C 177×10−4 Wm−1 K−1

at 100 ◦C 294×10−4 Wm−1 K−1

at 400 ◦C 805×10−4 Wm−1 K−1

Viscosity of liquidat mp 0.73mPa · sat bp 0.17mPa · sat 0 ◦C 0.07mPa · s

of gasat mp 36×10−4 mPa · sat 0 ◦C 93×10−4 mPa · sat 150 ◦C 143×10−4 mPa · s

Vapor pressureat −150 ◦C 0.002MPaat bp 0.102MPaat −50 ◦C 1.10MPaat 0◦ 4.27MPa

Explosive limits in air at0.1MPa and 20 ◦Clower (LEL) 2.75 vol % or 34.6 g/cm3

upper (UEL) 28.6 vol % or 360.1 g/cm3

Ignition temperature 425 – 527 ◦C

3. Chemical Properties

The chemical properties of ethylene result fromthe carbon – carbon double bond, with a bondlength of 0.134 nm and a planar structure. Ethy-lene is a very reactive intermediate, which canundergo all typical reactions of a short-chainolefin. Due to its reactivity ethylene gained im-portance as a chemical building block. The com-plex product mixtures that have to be separatedduring the production of ethylene are also dueto the reactivity of ethylene.

Ethylene can be converted to saturated hydro-carbons, oligomers, polymers, and derivativesthereof. Chemical reactions of ethylene withcommercial importance are: addition, alkyl-ation, halogenation, hydroformylation, hydra-tion, oligomerization, oxidation, and polymer-ization.

The following industrial processes are listedin order of their 1993 worldwide ethylene con-sumption [6]:

1) Polymerization to low-density polyethylene(LDPE) and linear low-density polyethylene(LLDPE)

2) Polymerization to high-density polyethylene(HDPE)

3) Addition of chlorine to form 1,2-dichloro-ethane

4) Oxidation to oxirane [75-21-8] (ethyleneoxide) over a silver catalyst

5) Reaction with benzene to form ethylben-zene [100-41-4], which is dehydrogenatedto styrene [100-42-5]

6) Oxidation to acetaldehyde7) Hydration to ethanol8) Reactionwith acetic acid and oxygen to form

vinyl acetate9) Other uses, including production of lin-

ear alcohols, linear olefins, and ethyIchlo-ride [75-00-3], and copolymerization withpropene to make ethylene – propylene (EP)and ethylene – propylene – diene (EPDM)rubber

4. Raw Materials

Table 1 lists the percentage of ethylene producedworldwide fromvarious feedstocks for 1981 and1992 [7]. In Western Europe and Japan, over80 % of ethylene is produced from naphthas –the principal ethylene raw materials.

A shift in feedstocks occurred for the pe-riod from 1980 to 1991. In the United Statesand Europe larger amounts of light feedstocks(LPG: propane + butane) and NGL (ethane, pro-pane, butane) are used for ethylene production,whereas in Japanmore naphthawas used in 1991compared to 1981. The use of gas oils for eth-ylene production decreased slightly during the1980s.

Ethane [74-84-0] is obtained fromwet naturalgases and refinerywaste gases. Itmaybe crackedalone or as a mixture with propane. Propane[74-98-6] is obtained from wet natural gases,natural gasolines, and refinery waste gases. Bu-tanes are obtained from natural gasolines andrefinery waste gases. A mixture of light hydro-carbons such as propane, isobutane [75-28-5],and n-butane [106-97-81], commonly called liq-uefied petroleum gas (LPG) and obtained fromnatural gasolines and refinery gases, is also usedas a feedstock.

Naphthas, which are the most importantfeedstocks for ethylene production, are mix-tures of hydrocarbons in the boiling rangeof 30 – 200 ◦C. Processing of light naphthas(boiling range 30 – 90 ◦C, full range naphthas(30 – 200 ◦C) and special cuts (C6 –C8 raffi-nates) as feedstocks is typical for naphtha crack-ers.

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Table 1. Raw materials for ethylene production (as a percentage of total ethylene produced)

Raw USA W. Europe Japan Worldmaterials 1979 1991 1981 1991 1981 1991 1981 1991

Refinery gas 1 3 2 17LPG, NGL 65 73 4∗ 14 10∗ 2∗ 31∗ 27Naphtha 14 18 80 72 90 98 58 48Gas oil 20 6 16 12 0 0 11 8

∗Including refinery gas

A natural-cut full-range naphtha containsmore than 100 individual components, whichcan be detected individually by gas chromatog-raphy (GC). Depending on the origin naphthaquality can vary over a wide range, which ne-cessitates quality control of the complex feedmixtures. Characterization is typically based onboiling range; density; and content of paraffins(n-alkanes), isoalkanes, olefins, naphthenes, andaromatics (PIONA analysis) by carbon num-ber. This characterization can be carried out byGC analysis or by a newly developed infraredmethod [8]. Full characterization of feedstocksis evenmore importantwhen production is basedon varying feedstocks, e.g. feedstocks of differ-ent origins purchased on spot markets.

The quality of a feedstock is depending onthe potential to produce the target products (eth-ylene and propylene). Simple yield correlationsfor these products can be used to express thequality of a feedstock in a simplefigure, the qual-ity factor, which indicates wether yields of thetarget products are high or low, with aromaticfeedstocks being poor and saturated feedstocksbeing good feedstocks.

Quality characterization factors for naphthashave been developed, which indicate the aro-matics content by empirical correlation. Sincearomatics contribute little to ethylene yields innaphtha cracking, a rough quality estimate canbe made for naphthas with a typical weight ratioof n- to isoparaffins of 1 – 1.1. The K factor isdefined as [9]:

K=(1.8Tk)1/3

d

where Tk is the molal average boiling point inK. Naphthas with a K factor of 12 or higher areconsidered saturated; those below 12 are consid-ered naphthenic or aromatic. The K factor doesnot differentiate between iso- andn-alkanes. TheU.S.Bureau ofMinesCorrelation Index (BMCI)

[10] can also be used as a rough quality measureof naphthas:

BMCI = 48640/T +473.7d−456.8

where T is the molal average boiling point inK and d is the relative density d15.6

15.6. A highvalue ofBMCI indicates a highly aromatic naph-tha; a low value, a highly saturated naphtha. Gasoils are feedstocks that are gaining importancein several areas of the world. Gas oils used forethylene production are crude oil fractions inthe boiling range of 180 – 350 ◦C (atmosphericgas oils, AGO) and 350 – 600 ◦C (vacuum gasoils, VGO). In contrast to naphtha and lightergas feeds, these feedstocks can not be character-ized by individual components.

Gas chromatography coupled with massspectrometry (GC –MS) or high performanceliquid chromatography (HPLC) allow the anal-ysis of structural groups, i.e., the percentage ofparaffins, naphthenes, olefins, monoaromatics,and polyaromatics in the gas oil, and can beused to determine the quality of the hydrocarbonfraction. If this information is used together withdata such as hydrogen content, boiling range, re-fractive index, etc., the quality canbedeterminedquite accurately. A rough estimate of feed qual-ity can be made by using the BMCI or the calcu-lated cetanenumber of a gas oil. The cetanenum-ber, normally used to calculate the performanceof diesel fuels, is an excellent quality measure,since it is very sensitive to the n-paraffin content,which is one of the key parameters for the ethyl-ene yield. The cetane number CN is calculatedas follows [11]:

CN= 12.822 + 0.1164CI + 0.012976 CI2

where CI = 0.9187 (T50 /10)1.26687

(n20D /100)1.44227, where T50 is the volume av-

erage boiling point in◦C and n20D the refractive

index at 20 ◦C

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5. Production

5.1. Ethylene from Pyrolysis ofHydrocarbons

The bulk of the worldwide annual commer-cial production of ethylene is based on ther-mal cracking of petroleum hydrocarbons withsteam; the process is commonly called pyrolysisor steam cracking. The principal arrangement ofsuch a cracking reactor is shown in Figure 1

A hydrocarbon stream is heated by heat ex-change against flue gas in the convection sec-tion, mixed with steam, and further heated to in-cipient cracking temperature (500 – 680 ◦C, de-pending on the feedstock). The stream then en-ters a fired tubular reactor (radiant tube or ra-diant coil) where, under controlled residencetime, temperature profile, and partial pressure,it is heated from 500 – 650 to 750 – 875 ◦C for0.1 – 0.5 s. During this short reaction time hy-drocarbons in the feedstock are cracked intosmaller molecules; ethylene, other olefins, anddiolefins are the major products. Since the con-version of saturated hydrocarbons to olefins inthe radiant tube is highly endothermic, high en-ergy input rates are needed. The reaction prod-ucts leaving the radiant tube at 800 – 850 ◦C arecooled to 550 – 650 ◦Cwithin 0.02 – 0.1 s to pre-vent degradation of the highly reactive productsby secondary reactions.

The resulting product mixtures, which canvary widely, depending on feedstock and sever-ity of the cracking operation, are then separatedinto the desired products by using a complexsequence of separation and chemical-treatmentsteps.

The cooling of the cracked gas in the trans-fer-line exchanger is carried out by vaporiza-tion of high-pressure boiler feed water (BFW,p= 6 – 12MPa), which is separated in the steamdrum and subsequently superheated in the con-vection section to high-pressure superheatedsteam (HPSS, 6 – 12MPa).

5.1.1. Cracking Conditions

Commercial pyrolysis of hydrocarbons to eth-ylene is performed almost exclusively in firedtubular reactors, as shown schematically in Fig-ure 1. These furnaces can be used for all feed-stocks from ethane to gas oil, with a limitation in

the end point of the feedstock of 600 ◦C. Higherboiling materials can not be vaporized under theoperating condition of a cracking furnace.

Increasing availability of heavy gas oil frac-tions, due to a shift in demand to lighter frac-tions, offers cost advantages for processingheavy feedstocks in some areas of the world.Furthermore, the availability of large quantitiesof residual oil have led some companies to in-vestigate crude oil and residual oils as ethyl-ene sources. Such feedstocks cannot be crackedin conventional tubular reactors. Various tech-niques employing fluidized beds, molten salts,recuperators, and high-temperature steam havebeen investigated, but none of these have at-tained commercial significance [12].

Pyrolysis of hydrocarbons has been studiedfor years.Much effort has been devoted tomath-ematical models of pyrolysis reactions for use indesigning furnaces and predicting the productsobtained fromvarious feedstocks under differentfurnace conditions. Three major types of modelare used: empirical or regression,molecular, andmechanistic models [13].

Today, mechanistic computer models, whichare available from various companies, are usedfor design, optimization and operation of mod-ern olefin plants. Sophisticated regression mod-els are also used, mainly by operators, and offerthe advantage of a much lower computer perfor-mance requirements than mechanistic models.

The regression models are based on a dataset, which can consist of historical data or cal-culated data. Depending on the quality of thedata base the empirical regressionmodels can beof sufficient accuracy for most operating prob-lems, within the range of the data field. Thesemodels can be run on small computers and arewell suited for process computer control and op-timization.

Molecular kineticmodels that use only appar-ent global molecular reactions and thus describethemain products as a function of feedstock con-sumption have been applied with some successto the pyrolysis of simple compounds such asethane, propane, and butanes.

For example, cracking of propane can be de-scribed as

C3H8 −→ aH2 + bCH4 + cC2H4

+ dC3H6 + eC4H8 + f C5+

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Figure 1. Principal arrangement of a cracking furnace

where a, b, c, d, e, f are empirical factors de-pending on the conversion of propane.

Gross oversimplification is required if thesemodels are applied to complex mixtures such asnaphthas or gas oils, but some success has beenattained even with these materials.

Advances have been made in mechanisticmodeling of pyrolysis, facilitated by the avail-ability of more accurate thermochemical kineticand pyrolysis data and of high-speed comput-ers. The major breakthrough in this area, how-ever, has been the development of methods tointegrate large systems of differential equations[14–16].

Mechanistic models need less experimen-tal data and can be extrapolated. The accuracyof these models is very good for most com-ponents, but they require permanent tuning ofthe kinetic parameters, especially for comput-ing the cracked-gas composition for ultrashortresidence times. Themain application for mech-anistic models is the design of cracking furnacesand complete ethylene plants. The accuracy ofthe models has been improved, driven by thecompetition between the contractors for ethyl-ene plants. A number of mechanistic models areused today in the ethylene industry, describing

the very complex kinetics with hundreds of ki-netic equations [17–19].

To demonstrate the complexity of the chem-ical reactions, the cracking of ethane to ethyl-ene is discussed here in detail. A simple reactionequation for ethane cracking is:

C2H6 −→ C2H4 +H2 (1)

If this were the only reaction, the product at100 % conversion would consist solely of eth-ylene and hydrogen; at lower conversion, eth-ylene, hydrogen and ethane would be present.In fact, the cracked gas also contains methane,acetylene, propene, propane, butanes, butenes,benzene, toluene, and heavier components. Thisreaction (Eq. 1) is clearly not the only reactionoccurring.

In the 1930s, the free-radical mechanismfor the decomposition of hydrocarbons was es-tablished [20]. Although the free-radical treat-ment does not explain the complete product dis-tribution, even for a compound as simple asethane, it has been extremely useful. Ethanecracking represents the simplest application ofthe free-radical mechanism. Ethane is split intotwo methyl radicals in the chain initiation step(Eq. 2). Themethyl radical reacts with an ethane

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molecule to produce an ethyl radical (Eq. 3),which decomposes to ethylene and a hydrogenatom (Eq. 4). The hydrogen atom reacts with an-other ethane molecule to give a molecule of hy-drogen and a new ethyl radical (Eq. 5).Initiation

C2H6 −→ CH•3 +CH•

3 (2)

Propagation

CH•3 +C2H6 −→ CH4 +C2H•

5 (3)

C2H•5 −→ C2H4 +H • (4)

H• +C2H6 −→ H2 +C2H•5 (5)

If reactions (4) and (5) proceed uninterrupted,the molecular reaction in Equation (1) results.If only reactions (3) – (5) occurred, the crackedgas would contain traces of methane (Eq. 3) andequimolar quantities of ethylene and hydrogenwith unreacted ethane. This is not observed.

Reactions (3) and (4) terminate if either anethyl radical or a hydrogen atom reacts with an-other radical or atom by reactions such as:Termination

H• +H• −→ H2 (6)

CH•3 +H• −→ CH4 (7)

H• +C2H•5 −→ C2H6 (8)

C2H•5 +CH•

3 −→ C3H8 (9)

C2H•5 +C2H•

5 −→ C4H10 (10)

On termination of chain propagation, newmethyl or ethyl radicals or a new hydrogen atommust be generated (Eqs. 2 – 4) to start a newchain. Thus, every time a new chain is initi-ated, a molecule of methane is formed (Eq. 3)and a molecule of ethylene is produced (Eq. 4).Other normal and branched-chain alkanes de-compose by a similar, but more complex, free-radical mechanism [21]. The number of possiblefree radicals and reactions increases rapidly aschain length increases.

The free-radical mechanism is generally ac-cepted to explain hydrocarbon pyrolysis at lowconversion [20]. As conversion and concentra-tions of olefins and other products increase,

secondary reactions become more significant.Partial pressures of olefins and diolefins in-crease, favoring condensation reactions to pro-duce cyclodiolefins and aromatics. The crackingof heavy feed, such as naphthas or gas oils, of-ten proceeds far enough to exhaust most of thecrackable material in the feedstock.

The reaction scheme with heavier feeds ismuch more complex than with gaseous feed-stocks, due to the fact the hundreds of reactants(feed components) react in parallel and some ofthose components are formed as reaction prod-ucts during the reaction. Since the radicals in-volved are relatively short lived, their concen-tration in the reaction products is rather low.

Radical decomposition is one of the most im-portant types of reaction and it directly producesethylene according to the following scheme:Radical decomposition

RCH2CH2CH•2 −→ RCH2

• +C2H4 (11)

This β-scission reaction produces a shorter rad-ical (RCH2

•) and ethylene. Radicals normallydecompose in the β-position, where the C –Cbond is weaker due to electronic effects. Largeradicals are more stable than smaller ones andcan therefore undergo isomerization.Radical isomerization

RCH2CH2CH•2 −→ RCH2CHCH3 (12)

The free-radical decomposition of n-butane(Eqs. 12 – 14) results in the molecular equation(Eq. 15):

n-C4H10 +H• −→ n-C4H•9 +H2 (14)

n-C4H9• −→ C2H4 +C2H5

• (15)

C2H•5 −→ C2H4 +H• (16)

n-C4H10 −→ 2C2H4 +H2 (17)

Reactions like (1) and (15) are highly en-dothermic. Reported values of ∆H at 827 ◦Care +144.53 kJ/mol for Equation (1) and+232.244 kJ/mol for Equation (15).

The mathematical description of these com-plex systems requires special integration algo-rithms [22]. Based on the pseudo steady stateapproximation, the chemical reactions can be in-tegrated and the concentration of all components

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at each location of the reactor (cracking coil) canbe computed [23], [24].

In a generalized and very simplified form thecomplex kinetics of cracking of hydrocarbons(ethane to gas oil) in steam crackers can be sum-marized as follows:Primary reactions Secondary reactionsFeedstock −→ ethylene −→ C4 products/steam propylene C5 products

acetylene C6 productshydrogen aromaticsmethane C7 productsetc. heavier products

The fundamentals of furnace design and themain influences of the different parameters canbe understood even with this simplified mecha-nism:

– Residence time: From the above scheme it isclear that a long residence time favors thesecondary reactions, whereas a short resi-dence time increases the yields of the pri-mary products, such as ethylene and propyl-ene.

– Partial pressure: Sincemost of the secondaryproducts result from reactions in which thenumber of molecules decreases, increasingthe pressure favors the secondary products.One function of the steam present in the sys-tem is to reduce the hydrocarbon partial pres-sure and thus favor the formation of primaryproducts.

– Temperature and temperature profiles: Theoligomerization reactions involved in theformation of secondary products are favoredby lower temperatures; therefore, specialtemperature profiles are applied along thecracking coil to avoid long residence timesat low temperatures.

Most commercial pyrolysis to produce eth-ylene is carried out in fired tubular reactors inwhich the temperature of the reactant increasescontinuously from the inlet to the outlet. Typicalinlet temperatures are 500 – 680 ◦C, dependingon the material being processed. Typical outlettemperatures are 775 – 875 ◦C.

Modern cracking furnaces are designed forrapid heating at the radiant coil inlet, where re-action rate constants are low because of the lowtemperature. Most of the heat transferred sim-ply raises the reactant from the inlet tempera-ture to the necessary reaction temperature. Inthe middle of the coil, the rate of temperature

rise is lower, but cracking rates are appreciable.In this section,the endothermic reaction absorbsmost of the heat transferred to the mixture. Atthe coil outlet, the rate of temperature rise againincreases but never becomes as rapid as at theinlet.

The designers of cracking coils try to opti-mize the temperature and pressure profiles alongthe radiant coils to maximize the yield of valu-able products yields by special coil design thatallows rapid temperature increase in the inletsection and low pressure drops in the outlet sec-tion of the cracking coils.

Typical process gas temperature profilesalong the radiant coil of modern ethylene fur-naces are shown in Figure 2 for ethane, propane,butane, and naphtha cracking.

The quantity of steam used, generally ex-pressed as steam ratio (kilograms of steam perkilogram of hydrocarbon), varies with feed-stock, cracking severity, and design of the crack-ing coil. Typical steam ratios used at a coil out-let pressure of 165 – 225 kPa (1.65 – 2.25 bar) forvarious feedstocks are:Ethane 0.25 – 0.35Propane 0.30 – 0.40Naphthas 0.4 – 0.50Atmospheric gas oils (cut: 180 – 350 ◦C) 0.60 – 0.70Hydrocracker bottoms (cut: 350 – 600 ◦C) 0.70 – 0.85

Steam dilution lowers the hydrocarbon par-tial pressure, thereby enhancing olefin yield. Italso reduces the partial pressure of high-boiling,high-molecular-mass aromatics and heavy tarrymaterials, reducing their tendency to depositand form coke in the radiant tubes and tofoul quench-exchanger tubes. Steam reduces thefouling of the radiant tubes by reacting with de-posited coke to form carbon monoxide, carbondioxide, and hydrogen in a water gas reaction,but as can be seen from the concentration of car-bon monoxide in the cracked gas (normally ca.100 ppm), only to a limited extent.

The sulfur content of the feed is important,since sulfur passivates active Ni sites of thecracking coil material by forming nickel sul-fides, which do not catalyze coke gasification,in contrast to nickel metal and nickel oxides.This explains why CO production is high (upto 1 % in the cracked gas) if the feedstock isfree of sulfur. To prevent this effect, ca. 20 ppmof sulfur (e.g., as dimethyl sulfide) are added tosulfur-free feedstocks.

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Figure 2. Process gas temperatures along radiant coils

Feedstock composition is another impor-tant consideration in commercial production ofethylene. Ethylene-plant feedstocks generallycontain straight- and branched-chain alkanes,olefins, naphthenes, and aromatics. Ethylene andother olefins are formed primarily from alkanesand naphthenes in the feed. n-Alkanes are thepreferred component for high ethylene yields,and those containing an even number of car-bon atoms give slightly better ethylene yieldsthan odd-numbered ones. n-Alkanes also pro-duce propene, whose yield decreases with in-creasing chain length.

Isoalkanes, in general, produce much smalleryields of ethylene and propene than n-alkanes.They give higher yields of hydrogen andmethane, and of C4 and higher olefins. Isoalka-nes tend to produce more propene than ethylenecompared to n-alkanes.

Olefin and diolefin yields from cyclopen-tane, methylcyclopentane, and cyclohexanehave been reported [21]; methylcyclopentaneand cyclohexane give substantial amounts of bu-tadiene.

Simple and condensed ring aromatics pro-duce no ethylene. Benzene is stable under nor-mal cracking conditions. It is formed duringcracking and remains unchanged in the feed.Other aromatics yield primarily higher molecu-lar mass components. Aromatics with long sidechains, such as dodecylbenzene, yield ethyleneand other olefins by side-chain cracking. Thearomatic nucleus still, however, generally pro-duces pyrolysis fuel oil and tar.

In summary, maximum ethylene productionrequires:

– A highly saturated feedstock– High coil outlet temperature– Low hydrocarbon partial pressure– Short residence time in the radiant coil– Rapid quenching of the cracked gases

These conditions maximize the yield ofolefins and minimize the yield of methane andhigh molecular mass aromatic components.

Cracking conditions and yield structure areoften optimized for economic reasons in plantdesign and operation; even small changes incracked gas composition influence the overallplant economics dramatically.

The dilution steam ratio is in most cases atthe minimum of the range for the specified feed-stock, due to the contribution of the dilutionsteam to the production costs.

5.1.2. Heat Requirements for HydrocarbonPyrolysis

Primary hydrocarbon pyrolysis reactions are en-dothermic; heat requirements are determined byfeedstock and cracking conditions. The temper-ature required to attain a given reaction rate de-creases as the carbon chain length in the feed-stock increases. Thus, the enthalpy required toreach cracking temperature depends on feed-stock and cracking conditions.

Heat requirements for hydrocarbon pyrolysiscan be divided into three components:

1) The enthalpy required to heat the feedstock,including the latent heat of vaporization ofliquids

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2) The endothermic heat of cracking3) The enthalpy required to heat the cracked gas

from the radiant-coil inlet temperature to theradiant-coil outlet temperature

The first is accomplished in the convection sec-tion of the furnace; the last two, in the radiantsection. Enthalpies (1) and (3) can be calculatedfrom standard heat-capacity data; they represent25 – 60 % of total process heat input in the fur-nace as the feedstock changes from ethane to gasoils [21].

A typical heat balance for a modern naphthafurnace including the TLE is shown in Figure 3.

The endothermic heat of cracking is mostsimply calculated from heats of formation bythe following equation:

∆Hr= ∆Hp−∆Hf

where ∆Hr = endothermic heat of cracking,kJ/kg; ∆Hp = heat of formation of the crackedproducts, kJ/kg; and ∆H f = heat of formationof the feed, kJ/kg. Heats of formation for somealkanes, olefins, naphthenes, and aromatics areas follows (in kJ/kg) [25]:

Hydrogen 0.0Methane −5646.3Ethane −3548.1Ethylene 1345.3Acetylene 8540.7Propane −2949.9Propene −17.9Methylacetylene 4317.1Propadiene 4496.8n-Butane −2694.4Isobutane −2827.51-Butene −459.4cis-2-Butene −649.5trans-2-Butene −668.2Isobutylene −746.5Ethylacetylene 2720.41,3-Butadiene 1721.8Benzene 783.6Toluene 243.4Cyclopentane −1611.3Methylcyclopentane −1722.6Cyclohexane −1846.4Methylcyclohexane −1890.3

As the alkane chain length increases, the heatof formation approaches 1800 kJ/kg asymptot-ically. Ethane, the most refractory alkane be-sides methane, has the most endothermic heat ofcracking, +4893 kJ/kg. The corresponding fig-ure for propane is +4295 kJ/kg and for a high-molecular-mass n-alkane, ca. 1364 kJ/kg.

Endothermic heat of cracking increases withdegree of saturation of the feed; as conversion

increases, secondary condensation products in-crease. These products have less negative heatsof formation than alkanes, or positive heats offormation.

5.1.3. Commercial Cracking Yields

Determining the complete yield patterns (gasand liquid products) for a commercial crackingfurnace requires a standardized procedure, espe-cially if the feedstock is changed from ethane tonaphtha and gas oil. A homogeneous sample iswithdrawn from the furnace effluent, quenched,and separated into gaseous and liquid fractions.These are analyzed separately and then com-bined to give a complete cracked-gas analysis.

Thematerial balance is obtained bymatchingthe hydrogen, carbon, and sulfur content of thefeedstock with that of the cracked gas. This typeof analysis is time-consuming. In a faster sys-tem, gas – liquid separation is eliminated [26] oronly a gas-phase analysis is taken. Due to manysources of errors, series of samples have to betaken and analyzed. Statistical methods are usedto check the quality of the results.

For gas feedstocks, conversion is used as ameasure of the severity of cracking:

Conversion =(Cn,in − Cn,out/Cn,in

)

where Cn,in = quantity of component n at inletin kg/h and Cn,out = quantity of component n atoutlet in kg/h. For liquid feedstocks the severityis defined as the ratio of propylene to ethylene(on weight basis) P/E or as ratio of methane topropylene M/P. Both ratios P/E and M/P are alinear function of temperature over a wide rangeand can bemeasured withmuch higher accuracythan the apparent bulk coil outlet temperature ofa cracking furnace.TheuseofP/EandM/P ratiosfor severity definition is accepted in industry.

Ethane. Ethane is cracked commercially inall types of furnaces, from long residence timeto short residence time. However, since ethane isa very stable paraffin, cracking temperatures atthe coil inlet typically are higher than for otherhydrocarbons. For ethane the coil inlet temper-atures are in the range of 650 – 680 ◦C. Typicalconversion ranges of commercial furnaces are60 – 70 %, with 67 % conversion being a typicalfigure for modern designs.

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Figure 3. Heat balance of a naphtha cracking furnace

Table 2 lists yields for ethane cracking at var-ious residence times. There is a slight increase inyield at short residence times. However, as therun length of short-residence-time ethane fur-naces is very low (Fig. 4) and yield improvementis moderate, application of short-residence-timefurnaces for ethane cracking is not feasible.

Figure 4.Run length versus residence time for ethane crack-ing

In naphtha plants the ethane contained in thecracked gas is separated and recycled to a segre-gated ethane-cracking furnace, in which crack-ing is carried out under typical ethane-cracking

conditions. In case the capacity of the ethanefurnace is not sufficient to crack all the ethane,cocracking of ethane with naphtha is performed,with ethane conversions of 40 – 50%. Due to thebuild up of large recycle streams in such oper-ations, cocracking should be avoided whereverpossible.

Propane is cracked in all types of furnacesat typical conversions of 90 – 93 %. The ap-plication of short-residence-time furnaces forpropane cracking has to be evaluated carefully,due to the dramatic reduction in run lengthbetween successive decokings. In many naph-tha plants with propane recycle, propane is co-cracked together with naphtha, without a dra-matic drop in propane conversion.

Typical yields for propane cracking for var-ious residence times are listed in Table 3. Forvery mild propane cracking conditions (70 %conversion) yields of propylene show a maxi-mum at 18 – 19 wt% based on propane feed.

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Table 2. Yields from ethane cracking with various residence times

Conversion, kg/kg 65.01 64.97 65.01 65.01Steam dilution, kg/kg 0.3 0.3 0.3 0.3

Residence time, s 0.4607 0.3451 0.186 0.1133

H2 wt% 4.04 4.05 4.09 4.12CO wt% 0.04 0.04 0.03 0.03CO2 wt% 0.01 0.01 0.01 0.01H2S wt% 0.01 0.01 0.01 0.01CH4 wt% 3.75 3.52 3.19 2.84C2H2 wt% 0.44 0.47 0.54 0.75C2H4 wt% 51.88 52.31 52.85 53.43C2H6 wt% 34.99 35.03 34.99 34.99C3H4 wt% 0.02 0.02 0.02 0.02C3H6 wt% 1.22 1.13 1.06 0.97C3H8 wt% 0.12 0.12 0.12 0.13C4H4 wt% 0.05 0.05 0.05 0.06C4H6 wt% 1.80 1.80 1.79 1.65C4H8 wt% 0.19 0.19 0.18 0.16C4H10 wt% 0.21 0.21 0.21 0.22Benzene wt% 0.55 0.47 0.38 0.26Toluene wt% 0.08 0.07 0.06 0.04Xylenes wt% 0.00 0.00 0.00 0.00Ethylbenzene wt% 0.01 0.00 0.00 0.00Styrene wt% 0.03 0.02 0.02 0.01Pyrolysis gasoline wt% 0.35 0.32 0.29 0.24Pyrolysis fuel oil wt% 0.21 0.16 0.11 0.06Sum wt % 100.00 100.00 100.00 100.00

Table 3. Yields from propane cracking with various residence times

Conversion, kg/kg 90.020 90.035 89.926 89.983Steam dilution, kg/kg 0.3 0.3 0.3 0.3

Residence time, s 0.4450 0.3337 0.1761 0.1099

H2 wt% 1.51 1.55 1.61 1.68CO wt% 0.04 0.04 0.03 0.04CO2 wt% 0.01 0.01 0.01 0.01H2S wt% 0.01 0.01 0.01 0.01CH4 wt% 23.43 23.27 22.82 22.40C2H2 wt% 0.46 0.51 0.59 0.82C2H4 wt% 37.15 37.51 38.05 38.59C2H6 wt% 3.06 2.80 2.37 1.96C3H4 wt% 0.52 0.57 0.65 0.89C3H6 wt% 14.81 14.82 15.01 15.27C3H8 wt% 9.97 9.96 10.07 10.01C4H4 wt% 0.08 0.08 0.09 0.11C4H6 wt% 2.85 2.9 2.98 2.99C4H8 wt% 1.00 1 1.02 1.09C4H10 wt% 0.04 0.04 0.05 0.05Benzene wt% 2.15 2.12 2.02 1.80Toluene wt% 0.43 0.4 0.36 0.28Xylenes wt% 0.05 0.05 0.04 0.03Ethylbenzene wt% 0.01 0.01 0.01 0.00Styrene wt% 0.21 0.2 0.18 0.15Pyrolysis gasoline wt% 1.27 1.26 1.27 1.24Pyrolysis fuel oil wt% 0.94 0.89 0.76 0.58Sum wt % 100.00 100.00 100.00 100.00

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Butane. All types of furnaces can be used forbutane cracking, which typically is performed at94 – 96 % conversion. Yields for n-butane andisobutane differ widely. For n-butane, ethyleneyields in the range of 40 % are typical (Ta-ble 4), whereas for isobutane only 15 wt% eth-ylene yield is achieved. Due to the poor ethyl-eneyield from isobutane, other applications suchas dehydrogenation, oligomerization, and alkyl-ation seem to be more feasible than crackingisobutane to produce ethylene. However, mildcracking at 70 % conversion and high pressureshas been claimed to yield isobutene as primaryproduct [27].

Naphtha. Naphtha, the refinery hydro-carbon fraction with the boiling range of35 – 180 ◦C, can vary in composition and boilingrange, depending on source and refinery con-ditions. Today naphtha cuts from 35 to 90 ◦C(light naphtha), 90 – 180 ◦C (heavy naphtha) and35 – 180 ◦C (full-range naphtha) are processed.In Europe and Asia/ Pacific naphtha is the pri-mary raw marerial for ethylene cracking, withfull range naphthas being processed most.

The properties of the naphtha feed stock usedto generate the yield patterns given in Tables 5,6, and 7 are as follows:Density at 20 ◦C 0.692 g/mLS content 55mg/kgH content 15.17wt%C content 84.80wt%Average molar mass 92 g/molBoiling curve (ASTM D 86)initial boiling point 26 ◦C5 vol % 49 ◦C10 vol % 53 ◦C20 vol % 58 ◦C30 vol % 64 ◦C40 vol % 70 ◦C50 vol % 77 ◦C60 vol % 86 ◦C70 vol % 99 ◦C80 vol % 116 ◦C90 vol % 138 ◦C95 vol % 152 ◦Cfinal boiling point 183 ◦CPIONA analysisn-Paraffins 36.13wt%Isoparaffins 36.62wt%Olefins 0.21wt%Napthenes 21.06wt%Aromatics 5.98wt%

Theyield increaseswith decreasing residencetime. The maximum benefit of a selective crack-ing coil is achieved in high-severity cracking, inwhich a 5 % feedstock saving can be achievedby using short residence times. However, careful

analysis is required since, similar to gas crack-ing, shorter run lengths are typical for short-residence-time cracking. Maximum annual fur-nace productivity is achievedwith a combinationof short residence time and long run length.

Gas Oil (AGO; Boiling Range180 – 350 ◦C). Compositions and boilingranges of gas oils vary greatly with source andrefinery conditions. Saturated gas oils may haveBMCI values as low as 20, whereas aromaticgas-oil BMCI values can exceed 45. Typicalyield distributions are shown in Table 8 for anAGO with properties as listed in Table 9.

Gas oils produce much more C5+ materialthan the above feedstocks because they containlarge amounts of condensedpolynuclear aromat-ics. These components resist cracking and mayremain unchanged or condense to higher molec-ular mass materials.

Hydrocracker Residue (HVGO or HCR;Boiling Range 350 – 600 ◦C). Hydrocrackerresidues are the unconverted product fractionfrom hydrocrackers. Due to the severe operatingconditions of the hydrocrackers, HCR is a highlysaturated product, with only a limited contentof aromatics and low contents of polyaromatics.HCR or HVGO is a feedstock that can result inethylene yields as high as in naphtha cracking.Typical yields for a HCR are shown in Table 8for an AGO with properties as listed in Table 9.

A comparison of the feedstock requirementsas a function of residence time for a 500 000 t/aplant for ethane, propane, butane and naphtha isshown in Figure 5. It can be seen that a naph-tha cracker has about three times the feedstockthroughput of an ethane cracker, and that naph-tha cracking shows some sensitivity to short res-idence times, whereas ethane crackers are notvery sensitive with respect to feedstock savingsas short residence times are applied. A carefuleconomic analysis is required to select the op-timum residence time range for a given feed-stock, since shorter residence times lead to re-duced availability due to shorter run length, asshown for ethane cracking in Figure 4.

5.1.4. Commercial Cracking Furnaces

Furnace Design. Modern cracking furnacestypically have one or two rectangular fire-

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Table 4. Yields from butane cracking with various residence times

Conversion, kg/kg 93.95 93.43 93.44 93.92Steam dilution, kg/kg 0.35 0.35 0.35 0.35

Residence time, s 0.4775 0.3440 0.1781 0.1117

H2 wt% 1.05 1.09 1.16 1.22CO wt% 0.04 0.04 0.03 0.04CO2 wt% 0.01 0.01 0.01 0.01H2S wt% 0.01 0.01 0.01 0.01CH4 wt% 20.48 20.29 19.85 19.33C2H2 wt% 0.37 0.42 0.51 0.71C2H4 wt% 35.03 35.81 37.25 38.36C2H6 wt% 4.57 4.16 3.47 3.02C3H4 wt% 0.87 0.93 1.04 1.32C3H6 wt% 17..37 17.24 17.03 16.99C3H8 wt% 0.37 0.35 0.33 0.33C4H4 wt% 0.09 0.1 0.11 0.13C4H6 wt% 3.98 4.08 4.27 4.38C4H8 wt% 2.85 2.83 2.78 2.85C4H10 wt% 6.05 6.07 6.06 6.08Benzene wt% 2.78 2.69 2.52 2.18Toluene wt% 0.83 0.77 0.66 0.49Xylenes wt% 0.12 0.11 0.09 0.06Ethylbenzene wt% 0.01 0.01 0.01 0.01Styrene wt% 0.25 0.24 0.22 0.18Pyrolysis gasoline wt% 1.85 1.81 1.80 1.72Pyrolysis fuel oil wt% 1.02 0.94 0.79 0.58Sum wt % 100.00 100.00 100.00 100.00

Table 5. Yields from low-severity naphtha cracking

P/E ∗, kg/kg 0.65 0.65 0.65 0.65Steam dilution, kg/kg 0.4 0.4 0.4 0.4

Residence time, s 0.4836 0.3526 0.1784 0.1096

H2 wt% 0.82 0.83 0.85 0.86CO wt% 0.03 0.02 0.02 0.02CO2 wt% 0.00 0.00 0.00 0.00H2S wt% 0.00 0.00 0.00 0.00CH4 wt% 13.56 13.2 12.44 11.83C2H2 wt% 0.32 0.34 0.36 0.45C2H4 wt% 25.23 25.6 26.08 26.43C2H6 wt% 4.76 4.36 3.62 3.16C3H4 wt% 0.59 0.63 0.70 0.92C3H6 wt% 16.42 16.63 16.97 17.18C3H8 wt% 0.68 0.65 0.61 0.60C4H4 wt% 0.09 0.09 0.10 0.12C4H6 wt% 4.63 4.86 5.27 5.68C4H8 wt% 5.76 5.94 6.34 6.69C4H10 wt% 0.72 0.75 0.80 0.85Benzene wt% 6.37 5.98 5.18 4.47Toluene wt% 3.08 2.9 2.60 2.26Xylenes wt% 1.17 1.15 1.09 0.96Ethylbenzene wt% 0.79 0.8 0.83 0.85Styrene wt% 1.08 1.01 0.87 0.77Pyrolysis gasoline wt% 11.25 11.81 13.19 14.09Pyrolysis fuel oil wt% 2.65 2.45 2.08 1.81Sum wt % 100.00 100.00 100.00 100.00

∗ Propylene to ethylene ratio, a measure of severity.

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Table 6. Yields from medium-severity naphtha cracking

P/E ∗, kg/kg 0.55 0.55 0.55 0.55Steam dilution, kg/kg 0.45 0.45 0.45 0.45

Residence time, s 0.4840 0.3572 0.1828 0.1132

H2 wt% 0.90 0.92 0.94 0.96CO wt% 0.04 0.04 0.03 0.04CO2 wt% 0.00 0.00 0.00 0.00H2S wt% 0.00 0.00 0.00 0.00CH4 wt% 15.23 14.91 14.31 13.82C2H2 wt% 0.44 0.47 0.53 0.71C2H4 wt% 27.95 28.45 29.24 29.87C2H6 wt% 4.59 4.23 3.57 3.14C3H4 wt% 0.71 0.76 0.87 1.21C3H6 wt% 15.38 15.64 16.09 16.43C3H8 wt% 0.53 0.51 0.48 0.47C4H4 wt% 0.12 0.13 0.16 0.20C4H6 wt% 4.54 4.79 5.28 5.79C4H8 wt% 4.41 4.52 4.75 4.95C4H10 wt% 0.42 0.44 0.47 0.49Benzene wt% 7.45 7.12 6.5 5.85Toluene wt% 3.26 3.10 2.82 2.46Xylenes wt% 1.18 1.16 1.12 0.97Ethylbenzene wt% 0.62 0.62 0.64 0.63Styrene wt% 1.21 1.14 1.00 0.88Pyrolysis gasoline wt% 7.70 7.96 8.52 8.79Pyrolysis fuel oil wt% 3.32 3.09 2.68 2.34Sum wt % 100.00 100.00 100.00 100.00

∗ Propylene to ethylene ratio, a measure of severity.

Table 7. Yields from high-severity naphtha cracking

P/E ∗, kg/kg 0.45 0.45 0.45 0.45Steam dilution, kg/kg 0.5 0.5 0.5 0.5

Residence time, s 0.4930 0.3640 0.1897 0.1170

H2 wt% 0.9 1.00 1.03 1.06CO wt% 0.06 0.06 0.05 0.06CO2 wt% 0.00 0.00 0.00 0.00H2S wt% 0.00 0.00 0.00 0.00CH4 wt% 16.9 16.61 16.10 15.74C2H2 wt% 0.64 0.69 0.80 1.14C2H4 wt% 30.25 30.81 31.74 32.38C2H6 wt% 4.32 4.00 3.43 3.00C3H4 wt% 0.81 0.88 1.02 1.48C3H6 wt% 13.63 13.88 14.29 14.55C3H8 wt% 0.37 0.35 0.33 0.32C4H4 wt% 0.18 0.2 0.24 0.32C4H6 wt% 4.20 4.45 4.90 5.39C4H8 wt% 3.11 3.17 3.26 3.28C4H10 wt% 0.17 0.18 0.19 0.18Benzene wt% 8.32 8.06 7.63 7.15Toluene wt% 3.40 3.26 3.00 2.63Xylenes wt% 1.14 1.12 1.09 0.95Ethylbenzene wt% 0.44 0.44 0.44 0.40Styrene wt% 1.44 1.37 1.24 1.12Pyrolysis gasoline wt% 5.25 5.35 5.55 5.57Pyrolysis fuel oil wt% 4.38 4.12 3.67 3.28Sum wt % 100.00 100.00 100.00 100.00

∗ Propylene to ethylene ratio, a measure of severity.

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boxes with vertical radiant coils located cen-trally between two radiant refractorywalls. Fire-box heights of up to 15m and firebox widths of2 – 3 m are standard design practice in the in-dustry. Firing can be performed with wall- orfloor-mounted radiant burners, or a combinationof both, which use gaseous or combined gaseousand liquid fuels. Fireboxes are under slight nega-tive pressures with upward flow of flue gas. Fluegas flow and draft are established by induced-draft fans. In some furnace designs, burners aremounted on terraced walls.

Table 8. Yields for AGO and HCR cracking

AGO HCR

P/E ∗, kg/kg 0.54 0.53Steam dilution, kg/kg 0.8 1

Residence time, s 0.32 0.3

H2 wt% 0.71 0.68CO wt% 0.01 0.01CO2 wt% 0.01 0.01H2S wt% 0.00 0.00CH4 wt% 10.58 11.08C2H2 wt% 0.38 0.60C2H4 wt% 25.93 25.98C2H6 wt% 2.82 2.81C3H4 wt% 0.63 0.97C3H6 wt% 14.07 16.02C3H8 wt% 0.37 0.42C4H4 wt% 0.12 0.04C4H6 wt% 5.73 8.03C4H8 wt% 3.61 4.14C4H10 wt% 0.05 0.06Benzene wt% 5.44 5.64Toluene wt% 3.49 2.73Xylenes wt% 0.92 0.46Ethylbenzene wt% 0.37 0.34Styrene wt% 1.18 1.12Pyrolysis gasoline wt% 7.28 6.91Pyrolysis fuel oil wt% 16.30 7.95Sum wt % 100 100

∗ Propylene to ethylene ratio, a measure of severity.

Firebox length is determined by the total eth-ylene production rate desired from each furnaceand the residence time of the cracking opera-tion. This also determines the number of indi-vidual radiant coils needed, with short residencetimes requiring many more individual coils thanlonger residence times for the same productioncapacity. This is due to the shorter lengths ofthe short-residence-time coils, which can be asshort as 10 – 16m per coil. Long-residence-timecoils can have lengths of 60 – 100mper coil. Thenumber of coils required for a given ethylene ca-pacity is determined by the radiant coil surface,

which is in the range of 10 – 15m2 per tonne offeedstock for liquid feedstocks.

Production rate for each coil is determinedby its length, diameter, and charge rate, whichtranslates into a certain heat flux on the radiantcoil. Values of 85 kW/m2 for the average heatflux of a coil should be the maximum.

Radiant coils are usually hung in a singleplane down the center of the firebox. They havealso been nested in a single plane or placed paral-lel in a staggered, double-row tube arrangement.Staggered tubes have nonuniform heat-flux dis-tributions because of the shadowing effect of onecoil on its companion. If maximum capacity andfull utilization of the firebox are desired, tubestaggering can be adjusted so that the shadow-ing effect is only marginally greater than with asingle-row arrangement.

Heat transfer to the radiant tubes occurslargely by radiation, with only a small contri-bution from convection. Firebox temperature istypically 1000 – 1200 ◦C.Table 9. Properties of AGO and HCR used for yield calculations inTable

AGO HCR

Density at 20 ◦C, g/mL 0.8174 0.8280C, wt% 86.20 85.28H, wt% 13.64 14.34S, wt% 0.18 0.003BMCI 24.8 9.37Paraffins + naphthalenes, wt% 80.38 89.4Monoaromatics, wt% 12.45 7.3Polyaroamtics, wt% 7.17 3.3Boiling point analysis, ◦Cibp 170 31310 % 203 35130 % 227 39350 % 248 40570 % 273 42290 % 316 45195 % 340 460fbp 352 475

The radiant coil of an ethylene furnace is afired tubular chemical reactor. Inlet conditionsmust meet the required temperature, pressure,and flow rate. Hydrocarbon feed is heated fromits convection-section entry temperature to thetemperature needed for entry into the radiantcoils. Dilution steam is introduced into the hy-drocarbon stream in the convection section. Thecombined hydrocarbon and steam stream is thensuperheated to the target temperature at the ra-diant coil inlet (crossover temperature, XOT).Gaseous feeds require only the energy necessaryto heat the feed and steam to the radiant coil in-

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let temperature. Liquid feeds require additionalenergy to heat the liquid to its vaporization tem-perature plus its latent heat of vaporization.

Figure 5. Feedstock requirements for a 500 000 t/a ethyleneplant

Energy is saved in the convection sectionby preheating the cracking charge; by usingutility preheating, i.e., boiler-feedwater preheat-ing, dilution-steam superheating, high-pressuresteam superheating or by preheating the com-bustion air.

A typical arrangement of furnace elementsis shown in Figure 6. In this case, the convec-tion section contains six separate zones. As anexample, the feed could be preheated in the up-per zone, the boiler feedwater in the next, andmixed feed and dilution steam in the third zone.The process steam is superheated in the fourthzone, the HP steam is superheated in the fifthzone and the final feed and dilution steam arepreheated in the bottom zone. The number ofzones and their functions can differ accordingto furnace design. For example, the upper zonecould be used to recover heat for air preheating.

With the trend to higher capacities per indi-vidual furnace a new furnace set-up has been in-troduced to the industry with great commercialsuccess. In this type two fireboxes are connectedto one convection section. This design allowsliquid feedstock cracking furnaces with capaci-

ties of 130 000 – 150 000 t/a to be installed. Thistwin radiant cell concept has been applied morethan 60 industrial furnaces since the late 1980s.

The induced-draft fans allow complex con-vection sections to be designed with very highgas velocities to give optimum heat transfer inthe convection section banks. Modern designsinclude integrated catalyst systems for NOx re-moval by SCR (selective catalytic reduction)technology, whereby the NOx present in the fluegas reacts with ammonia:

4NOx + 4NH3 +O2 −→ 4N2 + 6H2O

The temperature of the cracked gas leav-ing the radiant coils can range from 750 to900 ◦C. Rapid reduction of gas temperature to500 – 650 ◦C, depending on the feedstock, isnecessary to avoid losses of valuable productsby secondary reactions. This is accomplishedby a transfer-line exchanger (TLE) (see Fig. 6),which cools the cracked gases and recoversmuch of the heat contained in the cracked gasas high-pressure steam.

In all modern furnaces the radiant coils exitthe firebox at the top; the TLEs are top-mounted.In older designs coils also leave the bottom ofthe firebox, with TLEs mounted vertically alongthe side of the furnace or horizontally under-neath it. Radiant-coil designs are generally con-sidered proprietary information. All modern de-signs strive for short residence time, high tem-perature, and low hydrocarbon partial pressure.Most coil configurations have two features incommon: coils are hung vertically, usually sus-pended on spring or constant hangers above thetop of the radiant firebox, and they are fired fromboth sides of the radiant coil. Horizontal tubesare no longer used in ethylene furnaces.

Coils can range from a single, small-diametertube with low feed rate and many coils per fur-nace, to long, large-diameter tubes, with highfeed rate and few coils per furnace. Longer coilsconsist of lengths of tubing connected with re-turn bends. Individual tubes can be the samediameter or swaged to larger diameters one ormore times along the complete coil; two or moreindividual tubes may be combined in parallel.

An example of a so-called split radiant coilarrangement is shown in Figure 7; here parallelsmall-diameter coils are combined into a largerdiameter outlet coil. This arrangement allowsadvantageous temperature profiles to be applied,

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Figure 6. Typical arrangement of furnace elements

with a rapid temperature increase in the inlet sec-tion, and offers slightly higher yields than a uni-form diameter coil of the same residence time.

Figure 7. Short-residence-time coil arrangement

Coil lengths and diameters varywidely as canbe seen from the following design characteris-tics:

Ethylene capacity (per furnace) (50 – 130)× 106 t/aNumber of coils (per furnace) 4 – 200Tube diameter 25 – 180mmCoil length 10 – 100mCoil outlet temperature 750 – 890 ◦CTube wall temperatureclean 950 – 1040 ◦Cmaximum 1040 – 1120 ◦C

Average heat flux 50 – 90 kW/m2

Residence time 0.08 – 1.0 s

Cracking coils with internal fins have beenoffered to the industry, to increase the inner sur-face of a coil. These coils should offer the ad-vantage of processing more feedstock in a coilof identical external dimensions. However, thefins result in a higher pressure drop of the coil,with disadvantages in yields, and coke spallingproblems occurwhen the furnace is cooled down

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rapidly. Furthermore, the surface of a finned coilis of lower quality than that of a bare tube, andthis increases the coking rate of the finned tube.

Lummus Furnace (Lummus Crest, Bloom-field, N.J.). The coil design of Lummus fur-naces has beenmodified in the light of pilot-plantinvestigations. Six generations of coils SRT-I(short residence time-first model) through SRT-VI, have been produced.

The SRT-I model radiant coil is uniform indiameter. Many SRT-I heaters are still operat-ing, primarily for cracking ethane, propane, orbutane. All other coils are so-called split coils,with smaller inlet coils combined into larger out-let coils. The latest designs – SRT-V and SRT-VI – are short residence time coilswith residencetimes in the range of 0.15 – 0.20 s. In the SRT-Vcoil, 8 – 12 small coils of ca. 40mm internal di-ameter are headered into a single outlet coil oflarge diameter (150 – 180mm). In SRT-VI de-signs a smaller number of parallel coils is head-ered into a larger outlet tube, which is connectedto a linear quench exchanger.

Lummus furnaces can be paired, as shown inFigure 6, or can operate alone. Stacks may beshared, with a common induced-draft fan; theflue gas flows upward. Some convection sec-tions contain boiler feedwater preheating coilsand steam superheating coils, along with steamdesuperheat stations and process-heating coils.In some designs, steam is superheated in sep-arate heaters. Lummus heaters can be fired bywall-mounted burners or by combinations ofwall- and floor-mounted burners. Oil-fired floorburners are available.

Overall fuel efficiencies of 92 – 95 % netheatingvalue (NHV)canbeobtained, dependingon feedstock, fuel sulfur content, firing control,and convection section type. Lummus furnacescan use any available transfer-line exchanger.Radiant-coil outlets may be paired, leading to acommon exchanger. Capacities per furnace forfull-range naphtha or atmospheric gas oil varyfrom 25 000 to 100 000 t/a.

Millisecond Furnace (M. W. Kellogg Co.,Houston, Texas). The Millisecond Furnace isdesigned for shortest residence times and lowhydrocarbon partial pressures. It is recom-mended for gas and liquid feedstocks, offeringthe greatest advantages for the latter. This heater,

developed in the early 1970s from a prototypeinstalled by Idemitsu Petrochemical in Japan, re-duces residence time to ca. 0.10 s. Kellogg suc-cessfully marketed the Millisecond concept inthe mid-1980s, but with the trend of the industryto robust furnaces rather than maximum selec-tivity, which started in the 1990s, Kellogg lostmarket shares.

Figure 8. Kellogg Millisecond Furnace module ∗a) Preheated process fluid inlet; b) Radiant section; c) Ra-diant tubes; d) Convection section; e) Primary quench ex-changers; f) Induced-draft fan; g) Stack∗Reprinted with permission of M.W. Kellogg Co.

TheMillisecond Furnace uses Kellogg’s pro-prietary primary quench exchanger (PQE; seeSection 5.2). The furnace is decoked on-line byusing steam through the PQE and into the down-stream equipment. Coil outlet temperature is ca.50 ◦C higher than for competitive designs. TheMillisecond Furnace, which has a greater num-ber of smaller diameter and shorter tubes thanother furnaces designed for short residence time,is of modular design. Its capacity is increased byadding more units in series. Internal coil diam-eters are in the range of 30 – 40mm. A singlesmall PQE is fed by combining two or four ofthe small-diameter radiant tubes. Individual ra-

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diant tubes can number up to 200 per furnace,with 50 or 100 PQEs per furnace. Several PQEsare mounted in a single enclosure, for ease ofinstallation.

Furnaces can be paired to use a common steelstructure or they can stand alone. Paired furnacescan have a common stack and induced draft fan.Burners are located on opposite walls of the fire-box at floor level; they use gas, oil, or combina-tions thereof with forced or induced draft. Thedesign can be adapted easily for preheating com-bustion air. A Millisecond furnace is shown inFigure 8.

Flow is distributed to the many small-diameter radiant coils by pigtails connecting theindividual radiant coils to their common feedheader. Due to the short residence time andthe resulting higher process temperatures, runlengths of Millisecond furnaces are shorter thanthose of competing furnaces and they thus re-quire more decokes per year.

Stone & Webster Furnace (Stone & Web-ster Engineering Corp., Boston, Mass.). Stone& Webster supplies an ultraselective cracking(USC) furnace coupled with an ultraselectivequench exchanger (see Section 5.2). Radiantcoils have internal diameters of 50 – 90mm. Incontrast to many other contractors, Stone &Webster is not offering split coils.

Their swaged USC-U (Super U Coil) coilconfiguration consists of two tubes connectedwith a return bend. The diameter of the outlettube is larger than that of the inlet tube, allowingfor thermal, molecular, and pressure expansion.Generally, outlet tubes from two USC-U coilsare combined to feed a single ultraselective ex-changer (USX), but as many as four coils havebeen fed to a single USX.

Feed rates per radiant coil are low; individualfurnace capacity is increased by using as manyas 48 individual USC-U coils per furnace. TodayStone & Webster is offering Linear Exchangers(LinEx) instead ofUSXexchangers, for cost rea-sons.

The swaged USC-W coil configuration con-sists of four thin tubes, which differ in diameter.Individual diameters for each coil increase frominlet to outlet. A coil outlet can go directly to aUSX or LinEx quench system or two coils canshare a quench system. The individual furnacecapacity is obtained by installing 12 – 24 USC-

W coils in the same firebox. Spring hangers sup-port radiant coils from the top in the center planeof the firebox. Feed to the coils is equalized bycritical-flow venturi nozzles.

The USC furnaces may be paired as shownin Figure 5, with a common stack and induced-draft fan, or they can stand alone. Burners aremounted on the wall, or on the wall and floor.Floor burners are gas- or oil-fired.

For furnaces using gas-turbine integration(GTI) or preheating of combustion air, a floor-fired, short-residence-time (FFS) design is avail-able. This is completely floor fired, which re-duces large-volume ductwork to a minimum.Coil geometry is similar to USC-U or USC-Wdesigns, but to maintain a uniform firebox tem-perature, more and shorter coil legs are used.Overall fuel efficiencies of Stone&Webster fur-naces are competitive.

KTI Furnace (KTI Corp., The Hague, theNetherlands). A number of radiant-coil designsare available, ranging from a simple serpentinecoil of constant diameter to GK-1 (gradient ki-netics, model 1) and GK-5 coils.

Gaseous feed, naphtha, and gas oil can becracked with all coils. Residence times rangefrom 0.15 to 0.5 s. Capacities range up to120 000 t/a per furnace.

The GK radiant coil has two thin, paralleltubes from the coil inlet to ca. 66 % of the to-tal coil length, where they combine to a single,larger tube. The thin tubes can be staggered orin-line; the larger diameter tubesmust be in-line.

The KTI furnaces can be paired with acommon stack and induced-draft fan, or theycan stand alone. Top outlet coils are preferred.Burners are wall-mounted or wall- and floor-mounted.

Linde-Pyrocrack Furnace (Linde AG, Mu-nich, Germany). Linde-Pyrocrack furnaces pro-vide capacities of 20 000 – 130 000 t/a. Feed-stocks can be all straight-run or pretreated hy-drocarbons from ethane, propane, butane, natu-ral gas liquids, naphthas, raffinates, gas oils, gascondensates and hydrocracked vacuum gas oils.Furnaces are designed for segregated crackingor cocracking and for maximum feedstock flex-ibility. Linde and its U.S. subsidiary Selas FluidProcessing have installed furnaces with a totalethylene capacity > 13× 106 t/a.

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Figure 9. Linde-Pyrocrack coils

Pyrocrack coils are all split coils with smallinlet coils headered into a larger outlet coil, withresidence times from 0.15 to 0.5 s. The threebasic Pyrocrack coil types are shown in Fig-ure 9. Coil diameters range from ca. 40/55mm(inlet/outlet) for Pyrocrack 1-1 coils to 100/150mm for Pyrocrack 4-2 coils. Critical Venturinozzles are used to ensure equal distribution andresidence times in all parallel coils of a furnace.

Today almost exclusively a combination ofsidewall and floor firing is used, which offersthe best distribution of the released heat over thewhole firebox and a excellent radiant efficiency.Fuel for the radiant burners can be gas or oil orboth. Oil firing offers the opportunity to use afraction of the pyrolysis fuel oil (i. e., the liquidproduct of the pyrolysis boiling above 180 ◦C)as fuel and thus of increasing the amount of thepyrolysis methane fuel fraction available for ex-port to other comsumers.

The convection section of Linde Pyrocrackfurnaces contains process heating bundles forfeed, dilution steam, boiler feedwater, and high-pressure steam superheater bundles. Overall ef-ficiencies of up to 94 – 95 % (on lower heat-ing value, LHV) are typical for Linde furnaces.High-pressure steam systems for heat recovery

have been developed by Linde for up to 14MPa.Linde has built furnaces with SCR-based De-NOx technology integrated into the convectionsection. The design of the side and front wallsof the convection section provides uniform heatdistribution and prevents flue gas bypassing.Furnace draft is maintained by an induced-draftfan mounted over the convection section.

Linde has introduced with great commercialsuccess the Twin Radiant Cell concept, in whicha single high-capacity furnace has two radiantsections, which are connected to a common con-vection section (Fig. 10). Other new features area proprietary system for processing gas conden-sates, which have an extremely high and variablefinal boiling point. This system was developedfrom the well-established Linde technology forheavy hydrocracker bottoms and adapted to therequirements for gas condensates.

Linde is offering optimizers (OPTISIM) forthe optimization of the operation of furnaces andcomplete olefin plants.

Other Furnaces. The furnaces listed belowshow some interesting features, but none is ofcommercial importance in today’s worldwideolefin business. Only the furnace designs of

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Figure 10. Twin radiant cell furnace

the contractors listed above (Lummus, Kellogg,Stone & Webster, KTI, and Linde) are consid-ered to be competitive.

Figure 11. Foster –Wheeler terraced wall furnacea) Radiant coil; b) Burners

The terraced-wall furnace (Foster&WheelerEnergy Corp., Livingston, N.J.) uses burners fir-ing upward from shelves or ledges built into thewalls of the firebox (Fig. 11). A similar fireboxdesign is used for reformer heaters. This arrange-ment apparently gives uniform heating of the ra-

diant coil. Furnaces are all-gas or all-liquid fuelfired.

The Mitsui advanced cracker (Mitsui Engi-neering & Shipbuilding Co., Tokyo, Japan) of-fers lower construction costs, smaller land arearequirements, high thermal efficiency, and lowNOx emissions. The mass of steel used in a400 000 t/a ethylene plant is 30 % lower thanthat used in a 300 000 t/a plant with conventionalfurnaces. This is achieved by a patented instal-lation of three radiant coils in the firebox spacenormally occupied by one or two coils [28].

TheMitsubishi Furnace jointly developed byMitsubishi Petrochemical Co. and MitsubishiHeavy Industries of Japan is quite different in de-sign from other furnaces (Fig. 12). Known as theMitsubishi thermal cracking furnace (M-TCF),it is a vertical, downdraft furnace with the con-vection section located below the radiant fire-box. It is fired with gas or oil burners locatedin two rows mounted on the ceiling and tworows mounted on terraced walls. All burners aredown-firing, with long flat flames. According toMitsubishi, up to 70 % of the total heat can besupplied with any type of distillate fuel, includ-

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ing the cracked residue from an ethylene plant.Flue gas flows to a common stack by means ofan induced-draft fan, which produces suction atthe bottom of the convection section.

Figure 12. Section view of Mitsubishi M-TCF furnace ∗a) Flue-gas duct; b) Convection tubes; c) Side burners;d) Cracking coil; e) Roof burner; f) TLE∗Reprinted with permission of Mitsubishi Heavy Indus-tries.

5.1.5. Tube Metallurgy

Ample evidence indicates that maximum yieldsof ethylene from tubular cracking of hydrocar-bons require high temperature, short residencetime, and low hydrocarbon pressure in the radi-ant coil. Modified coils can help achieve theseconditions, but coil design is limited by metal-lurgy. Radiant coils must be selected in light ofthe following considerations:

– Operating temperature– Tube service life– Cost– Carburization resistance– Creep-rupture strength

– Ductility– Weldability

An outside tube wall operating tempera-ture up to and even exceeding 1100 ◦C isnow possible. Coils are designed to operate at975 – 1000 ◦C with an internally clean radiantcoil. Tube wall temperature rises with time be-cause of coke deposition inside the coil. Cokeacts as a thermal insulator inside the coil, requir-ing increased tube wall temperature for a givenfurnace loading. Localized overheating must beavoided during removal of coke from the coil(when steam or a mixture of steam and air isused). With steam-air decoking, combustion oc-curs inside the coils.

Tube service life is economically importantin plant operation. Furnace capital costs repre-sent ca. 20 % of the total cost of an ethyleneplant. About one-third of this is for radiant coils.With current metallurgy, a five-year service lifein the hottest section and a seven-year servicelife of the inlet section of a furnace are typical.Service life is shortened by carburization of theinner tube surface, which is favored by the envi-ronment inside a cracking coil. Temperature ishigh, and feeds are usually highly carburizing;reaction occurs between the gaseous phase in thetube and its base metal.

Coil alloys are normally protected by anoxide layer on the inner surface. If this layeris destroyed and cannot be regenerated, carbondiffuses into the basemetal, which itself diffusestoward the inside surface. Carburization may bemore severe during decoking and can be reducedby lowering the percentage of air mixed withsteam during this cycle. Aluminized coatings onthe inner surface of the tube may reduce carbur-ization [29–34]. The extent of carburization canbe measured by magnetic tests [32].

The materials used for cracking coils arehigh-alloy steels, e.g. with 35 % Ni, 25 % Crand several important trace metals (Si, Mn, Nb,Mo, W, Ti) [35]. The technical designation ofthis most common radiant coil material is HP 40modified. Only a limited number of manufac-turers worldwide are able to produce these ma-terials according to very strict quality standards.

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5.1.6. Thermal Efficiency of EthyleneFurnaces

Cracking furnaces represent the largest energyconsumer in an ethylene plant; their thermal effi-ciency is a major factor in operating economics.New plants are designed for 93 – 95 % thermalefficiency, and revamping of older ones can in-crease efficiencies to 89 – 92 %. Only a limitednumber of heat sinks are available for heat re-leased in the radiant firebox of a cracking fur-nace:

1) Process heat duty and duty for utility heating2) Wall or radiation loss3) Stack heat loss

Process heat duty is the energy required toheat the feedstock and dilution steam from thetemperature at which they enter the furnaceconvection section to the temperature at whichthey leave the radiant coil. Process heat dutyvarieswith feedstock composition, feed rate, andcracking severity. The duty for heating the util-ities is the heat requirement to heat boiler feed-water in the convection section (from 110 ◦C toca. 180 ◦C), before it is used for the HP steamproduction in the TLEs, and for superheating thesaturated HP steam produced in the TLEs in theconvection section.

Wall or radiation loss is that portion of theheat released in the radiant firebox which is lostto the atmosphere through the refractory andouter steel shells of the radiant and convectionsections. Wall loss is initially determined by thetype and thickness of thermal insulation in thefurnace. Typical wall losses in modern furnacesare 1.2 % of the fired duty for the radiant sectionand 0.3 % of the fired duty for the convectionsection.

Stack heat loss is that portion of the heat re-leased in the radiant firebox which is dischargedto the atmosphere in the flue gas. Stack heatlosses are around 5 % of the fired duty. Thisis the only heat loss that furnace operators cancontrol, given a fixed furnace design, quality ofmaintenance, feed rate, and coil outlet tempera-ture. Stack heat loss is sensitive to excess com-bustion air in the furnace and, thus, to draft, fuelcomposition, and air leakage.

Radiative Heat Transfer and FurnaceThermal Efficiency. The heat absorbed by the

radiant coils and lost through the walls of aradiant-section fireboxmust equal the heat givenup by the flue gas as it drops from the adiabaticflame temperature to the temperature at whichit leaves the firebox [36]. The heat absorbed bythe radiant coils of a furnace is a function ofcoil geometry, burner location, flame emissivity,temperature of the flue gas leaving the radiantfirebox, and tube wall temperature of the radiantcoil [37]. Typical radiant efficiencies are in therange of 38 – 42% for side wall firing, 40 – 45%for a combination of sidewall and floor firing and42 – 47% for 100% floor firing. The differencesresult from the direct radiation loss to the con-vection section if the burners are mounted in theupper section of the radiant box.

The effects of excess combustion air andcombustion air preheating on radiative heattransfer have been determined [38], [39]. Ex-cess air rates in modern furnaces are ca.10 %,but some plants are operated at rates as low as5 % excess air, resulting in reduced fuel con-sumption.

At 20 % excess combustion air (for a givenfurnace configuration and a radiant-section pro-cess duty), a 21% reduction in fuel consumptionis possible if combustion air is heated to 270 ◦C.Fuel usage increases rapidly as excess combus-tion air increases. At 49 % excess air, fuel con-sumption is the same as if combustion air werenot preheated.

Combustion air preheating may be used ina new ethylene plant or in a modernized fur-nace to increase thermal efficiency.Various heat-exchange techniques can be used, including di-rect exchange between flue-gas discharge andinlet combustion air by use of rotating refractoryvane elements, and indirect exchange by meansof heat pipes, high-pressure water, or circulatinghigh-temperature thermal fluids.

The most common technique for combustionair preheating is the use of hot exhaust gas fromgas turbines (GTs). Such plants co-produce elec-tricity (in the range of 30 – 60mWel.), and thishas a major impact on the plant economy. TheGTs are exclusively used for electricity produc-tion. Direct driving of large compressors by theGTs is not feasible, due to the maintenance re-quirements for GTs, which require an annualshutdown. In modern plants the ethylene plantcan run with and without the GT [40]. The econ-

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omy of operationwith an intregatedGT is highlydependent on the credit for the electricity and theincreased HP steam production. Scenarios thatfavor GT integration exist in Japan, Korea, andBrazil.

Radiant-coil inlet and outlet process temper-atures in an ethylene furnace must be the sameafter application of preheated combustion air asthey were before, to obtain the same crackingseverity.

Convective Heat Transfer and FurnaceThermal Efficiency. Convective heat transferis widely used in isolated green-fields ethyleneplants to improve thermal efficiency by preheat-ing boiler feedwater, generating steam, or super-heating HP steam in the convection section of afurnace. Recovered energy must be consideredin the overall energy balance for a plant of thistype. Such techniques can be employed in olderplants if boiler feedwater, generated steam, orsuperheated steam can be used. Otherwise, pre-heating the combustion air is an alternative.

5.1.7. Coking and Decoking of Furnaces andQuench Coolers

Radiant-Coil Coking. Hydrocarbon pyro-lysis produces acetylenic, diolefinic, and aro-matic compounds, which are known to depositcoke on the inside surface of the radiant coil [41],[42]. This coke layer inhibits heat transfer fromthe tube to the process gas, raises tube wall tem-perature, and reduces the cross-sectional flowarea of the tube, thus increasing the pressuredrop along the radiant coil. Cracking yield isthus lowered because of increasing hydrocarbonpartial pressure. When tube temperature lim-its are reached, or pressure limitations of thesonic venturi nozzles used for flow distribu-tion in short-residence-time furnaces, the fur-nace must be shut down to remove the coke.During the course of one on-stream cycle, de-posited coke can reduce the heat-transfer effi-ciency of the firebox by 1 – 2 %, resulting in a5 % increase in fuel consumption [43]. As radi-ant efficiency decreases, convection section heattransfer increases. This results in an unwantedincrease in process crossover temperature and alower demand for radiant-coil heat input. After

furnace firing equilibration, actual fuel demandincreases by 1 – 3 %.

Gaseous feedstocks such as ethane yield aharder, denser coke with higher thermal conduc-tivity than naphthas or gas oils. Highly aromaticfeeds produce the most coke.

The mechanism of coil coking is not fullyunderstood [44]. The possibility that tube met-als such as iron and nickel catalyze coke forma-tion is supported by the observation that sulfur inthe feed inhibits coking. A sulfur content above400 ppm, however, may increase coking.

Quench-Cooler Coking. Coke deposited intransfer-line exchangers (TLEs) reduces bothheat transfer and the amount of steam generatedto such an extent that the equipment must becleaned. Different mechanisms have been pro-posed for TLE coking or fouling [45]:

1) Spalled coke produced in the radiant coilis carried into the TLE inlet cone where itblocks some of the tubes on the TLE entrytube sheet. Such fouling is most serious inethane cracking.

2) Poor flowdistribution in the entry cone and atthe tube sheet causes eddies and backmixing.Gas so trapped experiences long residencetime at high temperature, which increases tarand coke production.

3) Heavypolynuclear aromatics andother high-boiling components in the cracked gas con-dense on the cool TLE tube walls. This isparticularly true for gas oil and heavy naph-tha feedstocks. The condensed high-boilingsubstances are gradually converted to coke-like materials. This mechanism is supportedby the fact that fouling is fastest at the start ofthe run (SOR). Typically, TLE outlet temper-atures increase by50 – 100 ◦Cduring thefirstday or two in gas oil cracking. Deposits dur-ing this period reduce the heat-transfer rate,and inner surface temperature at a given lo-cation in a tube becomes higher than the orig-inal clean wall temperature. The fouling ratedrops as the surface temperature increases;with time process gas temperature slowly in-creases.

Decoking. At some time, furnace operationthat is affected by coke deposits must be stoppedso that the coke can be removed. Mechanicaltechniques are not feasible. Usually, the coke

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is burned out with a mixture of steam and air(Fig. 13).

The furnace is taken off-line, the residual hy-drocarbons are purged downstream with steam,and the process flow is rerouted to a special de-coking system. A steam – air mixture is then in-troduced into the radiant coils to burn out thecoke at coil outlet temperatures of ca. 800 ◦C.The air concentration is increased carefully toavoid overheating the radiant coil. In modernfurnaces the CO2 content is measured contin-uously during decoking and the air flow rate isadjusted accordingly.After ca. 20 h the decokingof the radiant coils is complete and the decok-ing conditions are adjusted to decoke the TLE.Total decoking of radiant coil and TLE takes ca.36 h. Mechanical cleaning of the TLE is not re-quired in modern plant employing appropriatedecoking procedures.

Figure 13. Steam – air decoking

Steam-only decoking makes use of the wa-ter gas reaction, which is endothermic and lesslikely to burn out the radiant coils. This methoddoes not require the furnace to be discon-nected from downstream processing equipment,if that equipment is designed to accept the re-quired amount of steam and handle the carbonmonoxide produced. Temperatures as high as

950 – 1000 ◦C are required for steam-only de-coking. The decoking gas from the radiant coilsmaybe routed through the transfer-line exchang-ers, to partially decoke them.

Decoking time and radiant-tube wall tem-perature decrease as the amount of air mixedwith steam increases [46]. The result of a steam-only decoking operation is poorer than that of asteam – air decoke.

Modern furnace quench systems are designedso that off-gas from radiant-coil decoking passesdirectly through the transfer-line exchangers,which are decoked as a result. About once ayear a modern TLE must be opened for inspec-tion and cleaned mechanically. This is carriedout by shutting down the furnace, disconnectingthe TLE, and removing the coke from the tubesmechanically or hydraulically.

The furnace should never be shut down andcooled without radiant-coil decoking. Differ-ences between the coefficients of thermal ex-pansion of the coke and of the metal tube wallare such that the radiant coils may rupture.

Off-gas from decoking is usually diverted toa decoking system containing a knockout potequipped with a quench water inlet or a high-performance cyclone separator with dry or wetseparation of the coke particles in the effluent.The cleaned, cooled gases are discharged to theatmosphere. Alternatively, the decoke off-gascan be rerouted to the firebox, where the cokeparticles are incinerated.

5.2. Quenching of Hot Cracked Gas

Cracked gases leave the radiant coil of an eth-ylene furnace at 750 – 875 ◦C. The gases shouldbe cooled instantaneously to preserve their com-position. However, this is not practical, so fur-naces are designed to minimize residence timeof the hot gas in the adiabatic section betweenfurnace outlet and quench-system cooling zone.Typically, residence time in this adiabatic zoneshould not exceed 10 % of the residence time inthe radiant coil.

The cracked gas is generally cooled by in-direct quenching in the TLEs, which permitsheat recovery at a temperature high enough togenerate valuable high-pressure steam. Directquenching by injection of oil has been displacedalmost totally by indirect quenching.

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Design objectives for transfer-line exchang-ers are as follows:

1) Minimum residence time in the adiabaticsection between furnace outlet and TLEcooling surfaces, limiting secondary reac-tions that reduce the value of the cracked gas

2) Uniform flow to all tubes across the surfaceof the tube sheet, preventing eddies in theentry cone, which prolong residence time ofthe cracked gas and favor coke deposition.

3) Low pressure drop across the exchanger;pressure drop across the TLE is directly re-flected by the outlet pressure of the radiantcoil; increasing pressure at the outlet of theradiant coil degrades the value of the crack-ing pattern.

4) High heat recovery in the cracked gas, whichdirectly affects operating economics. Thepressure for steam generation is affected bythe cracking feedstock. For light hydrocar-bon cracking, in which little TLE foulingfrom condensation results, steam of muchlower pressure (60 bar) can be generated.With such feeds, two TLEs can be used in se-ries, one for generating high-pressure steam,the other for low-pressure steamor other heatrecovery. The TLE outlet temperature mustbe higher for liquid feeds (360 ◦C) becauseof condensation of heavy components in thecracked gas; therefore, the pressure of thegenerated steam can be higher (8 – 12MPa).In these cases, because of the high outlet tem-perature, TLEs are generally followed by adirect oil quench to lower the gas tempera-ture for entry into the downstream portion ofthe plant.

5) Reasonable TLE run lengths. Fouling ofTLE tubes by condensation and blockage bycoke increase outlet temperature and pres-sure drop. Ultimately, the system may haveto be shut down and cleaned. The TLE out-let temperature usually increases rapidly forseveral hours from the start-of-run (SOR)value; the increase then falls to a few ◦Cper day.

Figure 14 shows the TLE outlet temperatureover the run length for ethane, naphtha, andheavy feedstock (AGO, HVGO) cracking in amodern highly selective furnace.

The length of run for a TLE in gas crack-ing service is limited by coke blockage of the

TLE inlet tubes [44]. For liquid feeds, TLE runlength is governed by fouling at the outlet end ofthe tubes resulting from condensation of heavycomponents in the cracked gas. Fouling rate in-creases as boiling range and relative density ofthe feed increases.

Figure 14. Transfer-line exchanger outlet temperatures

The transfer-line exchangers with commer-cial importance are theBorsig exchangers (shell-and-tube and a double pipe closed coupled lin-ear exchanger), Schmidtsche (multi double pipeand a double pipe linear exchanger), the Stone& Webster USX exchanger and the Kellogg ex-changer (similar to the USX).

Borsig Transfer-Line Exchangers (Borsig,Berlin, Germany). The Borsig TLE design hasgained a large share of the world market (over50×106 t/a ethylene capacity) for use with feed-stocks ranging from ethane to atmospheric gasoils. Borsig offers two alternatives: a conven-tional shell-and-tube design and a linear ex-changer. The latest series of the shell-and-tubeexchanger, the tunnel-flow exchanger (Fig. 15),which was introduced in 1989, are specially de-signed to operate with large temperature andpressure differences across the hot-end tubesheet. This sheet is thin (ca. 15mm) but is sup-ported by a studded stiffening system. The mainfeature of the tunnel-flow exchanger is the con-trolled water flow pattern in the inlet section toavoid particle deposition on the tube sheet caus-ing hot spots.

Water flows from downcomers (a) into acircumferential water-jacket annulus (b). Fromhere water enters several parallel tunnels (c),which distribute thewater perfectly over the bot-tom tubesheet and via annular gaps in the stiffen-ing plate (e) to the individual tubes (d) contain-ing the hot cracked gas, which is cooled down

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Figure 15. Borsig tunnel-flow exchanger

by the water, producing high-pressure saturatedsteam.

Water flows through the tunnel system towardthe opposite side at high velocity in intimate con-tact with the tube sheet, thereby preventing de-position of solids. On the opposite side, waterflows upward through the circumferential annu-lus and enters the main shell volume (f). Debrismay be deposited on the outer edges of the tubesheet as water flows from it to the main shell,where blowdown nozzles are present. Minor de-posits here cause no problems because no heatload is present in this area.

Borsig exchangers can be mounted horizon-tally or vertically; the latter is the design for allmodern furnaces with a top-out concept. Out-let tube sheets are generally thick and uncooled.Thin, studded tube sheets may be needed forTLEs with high outlet temperatures, e.g., in gas-oil cracking [47].

A new development is the Borsig LinearQuencher, which is a double-pipe exchanger,connected directly to the coil outlet. This con-cept offers a minimum adiabatic volume of thecracking system.However, due to the larger tubediameter of this exchanger (up to 85mmod), theheat transfer is not as efficient as in the conven-tional system with smaller tubes. This translatesinto tube lengths of ca. 20m, which lead to thecharacteristic U shape of the linear exchangers,to keep the elevation of the steam drum within areasonable range. Due to the length of 20m, the

pressure drop is higher than in a conventionalsystem.

Figure 16 shows a Borsig Linear Quencher(BLQ) Themain features of the BLQ are the tur-boflow inlet chamber, with high water velocitiesto avoid solids deposition and a stepped bend atthe end of the primary leg to resist erosion in theU-shaped return bend.

Figure 16. Borsig Linear Quencher

Schmidt’sche Transfer-Line Exchang-ers (Schmidt’sche Heissdampf Gesellschaft,Kassel-Bettenhausen, Germany). SHGhas beendesigning transfer-line exchangers for ethylene

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crackers since 1960, with more than 3000 con-ventional and 400 linear exchangers supplied tothe industry up to 1996.

The SHG transfer-line exchanger shownin Figure 17 has separate exchangers, steamdrums, risers, and downcomers. The basic heat-exchange element consists of concentric tubes(a, b) welded at each end to oval tubes (c). Pro-cess gas flows through the inner tube, and wa-ter circulates through the annulus between thetubes.Many double-tube elements are combinedinto a single exchanger bywelding theoval head-ers to form a gastight tube sheet at each end.Process gas is delivered to the inner tubes of thebasic tube element by a specially designed entrycone (h), which provides uniform process gasflow through all tubes and reduces the probabil-ity of eddy formation in the cone. Process gasleaving the exchanger is collected in a conicalchamber and delivered to downstream equip-ment. Water flow to and from the oval tubesis provided by downcomers and risers (e) con-nected to the oval tubes by transition pieces (j).

Figure 17. SHG double-pipe transfer-line exchanger

The SHG transfer-line exchangers can bemounted vertically with upward or downwardflowof process gases. Theymayalso bemountedhorizontally with the gas-discharge end slightlyelevated with respect to the gas-inlet end. Theyare normally cleaned by steam – air decokingand from time to time cleaned by hydrojetting.

Schmidt’sche has also developed a closedcoupled linear exchanger, which offers a re-

duced adiabatic reaction zone, but due to the in-creased length has a higher pressure drop thanthe conventional exchanger. Figure 18 showsa Schmidtsche close coupled linear exchanger(SLE) in the typical U-shape. Feeds for allSchmidtsche exchangers range from ethane togas oils [48].

Figure 18. Schmidtsche close coupled linear exchanger

Stone & Webster Quench System (Stone& Webster Engineering Corp., Boston, Mass.).The Stone & Webster proprietary quench sys-tem does not rely on a tube sheet. The USX(ultra-selective exchanger) quench cooler shownin Figure 19 is a double-pipe exchanger, with theinner pipe slightly larger than the radiant-coilconnecting piping. This design can quench theeffluent from one to four radiant coils. The USXoutlet temperature (500 – 550 ◦C) is higher thanin most other transfer-line exchanger designs;this helps to reduce coking in the exchanger.Normally, effluents from all USX exchangers ona given furnace are combined downstream andfed to a conventionalmultitube exchangerwherethe gases are quenched to a more normal TLEoutlet temperature.

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This design, by eliminating the tube sheet andentry cone, eliminates turbulent eddies andback-mixing between the coil outlet and the coolingsurfaces, thereby reducing fouling in the TLEentry zone. The largeUSXgas flow tube reducespressure drop across the exchanger and, thus, theprobability of plugging by coke from the radiantcoil.

The USX exchangers can be steam – air de-coked; cleaning, when required, is facilitated byopenings at each end of the exchanger.

Figure 19.Ultraselective exchanger (USX) quench cooler ∗∗Reprinted with permission of Stone&Webster Engineer-ing Corp.

Kellogg Millisecond Primary Quench Ex-changer (M. W. Kellogg Co., Houston, Texas).A special primary quench exchanger (PQE) wasdeveloped for use with Kellogg’s Millisecondfurnace. The exchanger has a double-pipe ar-rangement (Fig. 20) capable of generating high-pressure steam.

A special high-alloy section of tubing is in-serted to avoid excessive thermal stress at thehigh-pressure steam transition piece. This sec-tion has the Y-fitting at its base and extends up tothe boiler feedwater inlet nozzle. A steam bleedhelps to control thermal gradients and to preventcoke deposition in the annulus between the high-alloy insert and the exchanger inner surface.

The steam system is a thermosiphon type,with individual risers and downcomers tied to-

gether in common headers connecting to a singlesteam drum. Kellogg’s PQEs are normally fab-ricated in bundles for ease of shipping and in-stallation. Typically, one PQE serves two coilsin a Millisecond Furnace.

Figure 20. Kellogg millisecond primary quench ex-changer ∗a) Y-shaped fitting; b) High-alloy insert; c) Double pipe∗Reprinted with permission of M.W. Kellogg Co.

Other Quench-Cooler Designs. Propri-etary quench coolers have been developed byLummus, Kellogg, C. F. Braun, Foster-Wheeler,and others.

The Lummus horizontal TLE, with conven-tional tube-and-shell exchanger design, can bemounted horizontally under the furnace firebox.It is used extensively in the United States andMexico for ethane cracking.

TheHitachi two-stage quench-cooler system(Hitachi, Japan) is similar to the Stone & Web-ster USX quench-system design. It consists of a

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primary double-pipe TLE for each furnace passor pair of passes, followed by a conventionaltube-and-shell TLE design capable of handlingthe combined process flow from all the primaryTLEs on a given furnace. Hitachi quench sys-tems have been used for cracking ethane, pro-pane, and full-boiling-range naphtha.

The Mitsubishi Quench Exchanger (Mit-subishi Petrochemical Co. and MitsubishiHeavy Industries of Japan) is available in twodesigns: M-TLX-I andM-TLX-II. TheM-TLX-I contains the transfer-line exchanger and thesteam drum as an integral unit. Up to four coiloutlets can be connected to a single M-TLX-I,if coil arrangement permits. TheM- TLX-ll alsohas on-line decoking capability if boiler feedwa-ter and hydrocarbon feed are removed from theexchanger. The M-TLX-II has a separate steamdrum.

Figure 21. Mitsui innovative quencher ∗a) Honeycomb tube nest; b) Inner tube; c) Heat-tranfertube; d) Outer tube; e) Steam drum∗Reprinted with permission of Mitsui Engineer-ing&Shipbuilding Co.

The Mitsui Quench Exchanger (Mitsui En-gineering & Shipbuilding Co., Tokyo, Japan)

(Fig. 21) uses an integrated exchanger, steamdrum, risers, and downcomers.

Cracked gas rises through spaces betweenmany heat-exchanger elements (c) suspendedfrom the tube sheet of the steam drum (e) andleaves the exchanger at the gas-outlet nozzle.Each heat-exchange element consists of a pairof concentric tubes. The inner tube (b) is openat the bottom end; the outer tube (d) is closed.Cooling water flows down the inner tube from areservoir in the center of the steam drum, leavesthe open end of the inner tube, and returns to thesteam drum via the annulus between the innerand outer tubes. Steam generated in the annu-lus is separated and dried in the upper sectionof the steam drum. This design eliminates prob-lems caused by differences in thermal expan-sion of the tubes. The system must be decokedon-line. Mechanical cleaning of the cracked-gasflow path is not possible. Up to six radiant coilscan be combined and served by one Mitsui TLEsystem [49].

5.3. Recovery Section

The cracked gas leaving the cracking furnacesmust be cooled to recover the heat it con-tains in the cracked gas and render it suitablefor further processing. The temperature of thecracked gas leaving the primary TLE dependson the feedstock type; it varies from 300 ◦C forgaseous feedstock, to 420 ◦C for naphtha feed-stock, and up to 600 ◦C for AGO and hydroc-racker residues. In ethane and propane cracking,cooling to ca. 200 ◦C is performed in heat ex-changers by preheating feedstock orBFW.How-ever, this step can not be done in heat exchang-ers for feedstocks heavier than propane, due tothe condensation of the liquid portion containedin the cracked gas. Cooling such cracked gasesto 200 ◦C would lead to excessive fouling ofthe heat exchangers by carbon deposits. Thus,cooling is performed by injection of oil into thecracked gas (oil quench) by means of specialtangential-injectionmixing devices.Oil quench-ing is performed individually for each furnace orin the combined cracked gas line after collectionof the cracked gas from all furnaces. In moderndesigns, the oil injection is located in the fur-nace area, integrated into the cracked gas linedownstream from the TLEs.

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The cracked gas leaving the furnace sec-tion has a temperature of ca. 200 – 250 ◦C andis routed to the separation section via a largecracked gas line. The collected gas stream con-tains the effluents of all cracking furnaces, in-cluding those processing recycle streams.

Table 10 shows the yields of the product frac-tions for all typical feedstocks. Apart from thetype of feedstock, the gas composition and,therefore, the design of the downstream recov-ery process also depends on the cracking severityand the applied coil design.

Further processing, i.e., separation into themain products or fractions, can be performedin different sequences and depends on the feed-stock type and the number and the specificationof the plant products. Themain downstreampro-cessing steps are the removal of the heat con-tained in the cracked gas, condensation of waterandheavyhydrocarbons, compression,washing,drying, separation, and hydrogenation of certainmultiply unsaturated components. Themain taskof these steps is to recover the desired productsat given specifications and at the desired battery-limit conditions.

Ethane, propane, and butane can be recycledto the furnace section to increase the overallyield of ethylene per tonne of feedstock pro-cessed. Processing differs for cracked gas de-rived from gaseous and liquid feedstocks, sincethe portion of heavy components increases, es-pecially when processing naphtha or even heav-ier feedstocks such as gas oil and hydrocrackerbottoms. When pure ethane is the feedstock,the amount of C3 and heavier byproducts issmall, and only rarely is the recovery of heav-ier products economically feasible. As the con-centration of heavier components increases, re-covering them for direct sale becomes feasible.Addition of significant amounts of propane toethane feedstock makes a depropanizer neces-sary and hydrotreating and fractionation of theC3 cut may be required; butane feeds make oiland gasoline removal from the cracked-gas com-pressor necessary; pentane-range feeds requirefractionation of light from tarry oils, and so on.

5.3.1. Products

Local market conditions and the degree of in-tegration of the ethylene units into refining or

petrochemical complexes influence the desiredproducts and the feedstocks used.Many types ofcoproduct can be generatedwith different equip-ment [50–52]; only the major product optionsare discussed here.

The principal ethylene coproducts are as fol-lows:

– Acetylenes (C2 and C3) are hydrogenated toethane, ethylene, propane, and propene; orthey may be recovered and sold as products.

– Aromatics (various fractions) can be reco-vered or theymay remain in the hydrotreatedpyrolysis gasoline.

– C4 olefins can be refined for butadiene, buty-lene, isobutylene, or mixtures thereof.

– C5 olefins can be either recovered and re-fined to give isoprene, piperylene, and cyclo-pentadiene, or hydrotreated in the pyrolysisgasoline fraction.

– Ethane is recycled as cracking feedstock orused as fuel.

– Fuel oil is used as such or to produce cokeor carbon black.

– Hydrogen is purified and used for hydrogen-ation steps in the plant; excess hydrogen issold or used as fuel in the plant.

– Methane is used as fuel or sold.– Naphthalene is recovered for sale or left inthe pyrolysis fuel oil fraction.

– Propane is recycled as a cracking feedstock,used as fuel, or sold.

– Propene is sold in various grades.– Rawpyrolysis gasoline is sold asmotor gaso-line after hydrotreatment, or it is used asfeedstock for aromatics production.

– Tar is sold for fuel, used as coke feedstock, ordiluted with hydrocarbon stocks to producefeedstocks for resins.

– Sulfur is recovered in some plants and sold.

5.3.2. Cracked Gas Processing

Many options are available for general processconfiguration [50], [53–59]. The sequence forisolation of hydrocarbon fractions can be var-ied, depending on plant size, amounts of ethyl-ene and coproducts, impurities, product range,product purity desired, and other factors.

The following discussion of the recovery pro-cess is split into two sections:

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Table 10. Cracking yields for various feedstocks

Ethane Propane Butane Naphtha AGO HCR

P/E ∗, kg/kg (65) ∗∗ (90.0) ∗∗ 0.35 0.55 0.54 0.53Steam dilution, kg/kg 0.3 0.3 0.487 0.45. 0.8 1

Residence time, s 0.3451 0.3337 0.344 0.3572 0.32 0.3

H2 wt% 4.05 1.55 1.09 0.92 0.71 0.68CO wt% 0.04 0.04 0.04 0.04 0.01 0.01CO2 wt% 0.01 0.01 0.01 0 0.01 0.01H2S wt% 0.01 0.01 0.01 0 0 0CH4 wt% 3.52 23.27 20.29 14.91 10.58 11.08C2H2 wt% 0.47 0.51 0.42 0.47 0.38 0.6C2H4 wt% 52.31 37.51 35.81 28.45 25.93 25.98C2H6 wt% 35.03 2.80 4.16 4.23 2.82 2.81C3H4 wt% 0.02 0.57 0.93 0.76 0.63 0.97C3H6 wt% 1.13 14.82 17.24 15.64 14.07 16.02C3H8 wt% 0.12 9.96 0.35 0.51 0.37 0.42C4H4 wt% 0.05 0.08 0.1 0.13 0.12 0.04C4H6 wt% 1.80 2.90 4.08 4.79 5.73 8.03C4H8 wt% 0.19 1.00 2.83 4.52 3.61 4.14C4H10 wt% 0.21 0.04 6.07 0.44 0.05 0.06Benzene wt% 0.47 2.12 2-69 7.12 5.44 5.64Toluene wt% 0.07 0.40 0.77 3.1 3.49 2.73Xylenes wt% 0.00 0.05 0.11 1.16 0.92 0.46Ethylbenzene wt% 0.00 0.01 0.01 0.62 0.37 0.34Styrene wt% 0.02 0.20 0.24 1.14 1.18 1.12Pyrolysis gasoline wt% 0.32 1.26 1.81 7.96 7.28 6.91Pyrolysis fuel oil wt% 0.16 0.89 0.94 3.09 16.3 7.95Sum wt % 100.00 100.00 100 100.00 100 100

∗ P/E = propylene to ethylene ratio, ∗∗Conversion of feedstock

1) Front-end section, including cracked gascompression and associated units

2) Hydrocarbon-fractionation section

Difference between the two sections is made forsimplicity reasons. The basic process route forthe front-end section is identical for all commer-cial processes, however major difference existsbetween gas- and liquid feedstock cracking. Forthe hydrocarbon fractionation section there area large variety of process routes available, whilethe feedstock type results only in minor differ-ences of the basic process route.

5.3.2.1. Front-End Section

The front-end section (Figs. 22, 23) receives theeffluent stream from the cracking furnaces. Itsmain task is to cool the cracked gas stream, re-covering waste heat and providing it to otherplant sections, to condense and to produce dilu-tion steam, and to remove heavy hydrocarboncomponents such as tar, oil, and heavy gaso-line. The resulting purified gas is compressed inthe cracked gas compression section and dried

to prepare it for further cryogenic separation inthe fractionation section. An acid-gas removalstep that eliminates all CO2 and H2S from thecracked gas is incorporated between the finalcompressor stages.

The process configuration of this front-endsection is fairly independent from licensers asthey all follow the same process principals.However there are many variations in detaileddesign. Major differences are observed betweenplants processing gaseous feedstocks (ethane,propane, and butane) and those treating liquidfeedstocks like naphtha. Processing of crackedgas resulting from liquid feedstocks is morecomplex as higher amounts of heavy hydrocar-bons are condensed and must be removed in thissection.

Process Description. The main differencebetween the process for gaseous feedstock(Fig. 22) and liquid feedstock (Fig. 23) is thepresence of a primary fractionator that removestar and oily material (bp > 200 ◦C) from thecracked gas in the latter. In the case of crackinggaseous feedstock only, this step is not neces-

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sary, as the small amounts of heavy hydrocar-bons present in the cracked gas can be removedin the water-quench column. Furthermore, ad-ditional installations are required in the water-quench system and in the compressor and dry-ing units to treat the larger amount of pyrolysisgasoline that condenses in these units.

Primary Fractionation. With liquid pyroly-sis feedstocks, the primary fractionation columnis the first step in the cracked gas processingroute. Cracked gas enters the column typicallyat 230 ◦C. In the column it is contacted with cir-culating oil and, at the top of the column, with aheavy pyrolysis gasoline fraction obtained fromthe subsequentwater-quench tower. Cracked gasleaves the top of the primary fractionator at ca.100 ◦C, free of oil but still containing all the di-lution steam. Hot oil, which functions as a heatcarrier, is collected at the bottom of the columnand, after cooling, recirculated as reflux to themiddle section of the primary fractionator andto the quench nozzles downstream of the TLEs.Most of the heat contained in the cracked gasleaving the TLE’s is removed by the circulatingquench oil. Heat is reused for generation of pro-cess steam as well as for other purposes suchas preheating of feedstock, preheating of pro-cess water, or for other energy consumers at anappropriate temperature level. Excess oil is re-moved from the primary fractionation systemand sent out as product. Pyrolysis oil is gen-erally produced as one fraction, containing allhydrocarbons boiling above 200 ◦C. Howeversome plants produce two qualities of pyrolysisoil, one called PGO (pyrolysis gas oil) boiling inthe range 200 – 400 ◦C and PFO (pyrolysis fueloil) containing the heavier components.

Water-Quench Column. The overhead ofthe primary fractionator is routed to the water-quench column, in which the cracked gas iscooled to near ambient temperature by contact-ing it with a large stream of circulating quenchwater. In this cooling step most of the dilutionsteam and a heavy gasoline fraction are con-densed and collected at the bottom. After grav-ity separation, heat is extracted in a circulat-ing loop and most of the water stream is usedto produce dilution steam. Large amounts oflow-temperature heat (60 – 80 ◦C) are recoveredand used for various heating purposes in the

recovery section. The largest consumer of thislow temperature heat is typically the reboiler ofthe propene – propane fractionation tower. Mostof the condensed gasoline is recycled as re-flux to the top of the primary fractionator. Theexcess gasoline fraction is sent to a gasolinehydrotreater or fractionated further into higherquality gasoline and heavier oil streams. Bothwater and gasoline fractions, except when frac-tionated further, are stripped of dissolved lightgases [50], [53], [60], [61].

In the case of processing cracked gas fromgaseous feedstock, the furnace effluent streamis directly fed to the quench tower after coolingin a secondary TLE to ca. 200 ◦C. In this case thesystem is simpler as no or only small amountsof tar and oil condense and must be removed.A general problem in all quench towers is theseparation of hydrocarbons and water. There isa strong tendency for formation of emulsions,leading to fouling problems in the generationof dilution steam and in the processing of thewastewater from the system. Emulsification isavoided by careful control of the pH value in thequench-water system.

Numerous options exist in the design and op-eration of the quench column and primary frac-tionator units for removing pyrolysis tars, recov-ering various heavy hydrocarbon streams, andisolating quench oil for recycle [50], [60], [61].

Dilution-Steam System. The dilution steamrequired in the cracking process forms a closedloop over the cracking furnaces and the quench-water column. Excess water from the bottomof the quench column is stripped in a processwater stripper to remove volatile hydrocarbons.Some 5 – 10 % of the process water is purged toavoid concentrating dissolved solids. The gen-eration of the process steam is typically per-formed at 800 kPa. In liquid feedstockprocesses,50 – 80 % of the dilution steam is generated byrecovering heat from the hot quench oil cyclefrom the bottom of the primary fractionator. Thebalance heat duty is provided by condensingsteam

Compression. After cooling and purificationof the cracked gas in the primary fractiona-tor and/or in the quench tower, further process-ing requires compression to ca. 3200 – 3800 kPa.Some condensation of water and hydrocarbons

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Figure 22. Simplified process flow diagram for the front-end process of an ethylene plant cracking gaseous feedstocks

Figure 23. Simplified process flow diagram for the front-end process of an ethylene plant cracking liquid feedstocks

occurs during compression, and in the laterstages, acidic gases are removed. Compressionis typically performed by a turbine-driven cen-trifugal compressor in four to six stages withintermediate cooling. The number of stages de-pends primarily on the cracked-gas compositionand the highest temperature allowed for inter-stage discharge. Interstage cooling and temper-ature control keep the cracked gas below 100 ◦Cto prevent diolefin polymerization and subse-quent equipment fouling. Various injection sys-tems, using aromatic rich oil or water, are ap-plied to reduce fouling of compressor internalsand intercooling equipment. Interstage coolingusually employs water coolers to minimize in-let temperature in the subsequent stages. First-stage compressor suction is normally main-tained somewhat above atmospheric pressure toprevent oxygen intrusion. The operating pres-sure is set to economically balance yield in thecracking coils against higher energy consump-tion for compression [50]. The compressor dis-charge pressure is set by the choice of refrigerantso that methane condenses in the demethanizer

overhead condenser. Condensation temperaturevaries with hydrogen/methane ratio. The dis-charge pressure,with the coldest ethylene refrig-erant level typically at ca. −100 ◦C, is normally3200 – 3800 kPa. The criteria used to determinesuction pressure and discharge pressure are se-lectivity and energy consumption [50], [61].

Interstage cooler pressure drops must be keptlow, especially in the initial stages, to reducecompressor and energy costs. The water and hy-drocarbon condensates may be routed to anothercompressor stage, to the primary fractionatorpreceding the compressor, or to a fractionationtower. In liquid cracking most of the gasolinefraction containing the C6 to C8 aromatics iscondensed in the interstage coolers of the com-pressor. After gravity separation from processwater this gasoline stream is fractionated in astripper to remove C4 and lighter componentsbefore routing it to a hydrotreating step. Dryingis required for all liquid and gas streams sub-jected to temperatures below 15 ◦C [50], [53],[59], [60].

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The acid-gas removal system is typically lo-cated between the 3rd and 4th, or between the4th and 5th stages. Some fractionation processesthat have deethanization or depropanization asthe first process stage have this fractionation stepbetween the 4th and 5th compressor stages. Inthese cases moisture must be removed upstreamof the fractionation step to avoid formation ofhydrates and ice.

Acid-Gas Removal. Before further process-ing, carbon dioxide and hydrogen sulfide are re-moved from the cracked gas by once-throughand regenerative solvent scrubbing. Sulfur mayalso be removed from the cracker feedstock [50].

Acid gas is usually removed just before the4th or 5th compression stage. Carbon dioxide isremoved because it can freeze at low tempera-ture in heat-exchange and fractionation equip-ment. Carbon dioxide can also be absorbed intoethylene, affecting product quality and furtherprocessing. Hydrogen sulfide is corrosive anda catalyst poison as well as a potential productcontaminant [52], [53].

These acid gases are scrubbed with sodiumhydroxide on a once-through basis or in combi-nation with a regenerative chemical. Regenera-tive prescrubbing before final sodium hydroxidetreatment is common in large cracking plants,especially those that use high-sulfur feedstocks.This reduces sodium hydroxide consumption,which is desirable for economic and environ-mental reasons.

Regenerative scrubbing can employ alka-nolamines, but it is not possible with this treat-ment alone to lower the concentration of CO2 tothat required to protect high-activity polymer-ization catalysts against CO2 poisoning (e.g., to0.2 ppm). Use of regenerative scrubbing is typ-ically limited to liquid-cracking operations. Inany case a polishing scrubber consisting of acaustic wash unit is applied to achieve the re-quired CO2 specification in the effluent stream.Acid-gas removal systems are frequently subjectto fouling, especially at high concentrations ofC4 and C5 diolefins. The fouling process can becontrolled by applying special inhibitors.

Acid gases liberated from the regenerativesolvent can be incinerated or recovered [50],[53], [60], [61], [62]. Waste caustic, containingsulfides in the range of a few % is usually oxi-

dized and neutralized in a wet caustic oxidationunit or neutralized and stripped, before feedingit to the sewer system.

Drying. The cracked gas is saturated withwater before compression and after each inter-cooler stage. Moisture must be removed beforefractionation to prevent formation of hydratesand ice. Typically, this is accomplished by chill-ing and by adsorption onmolecular sieves.Olderplants also used absorption by aglycol scrubbingsystem or adsorption on alumina [52]. Drying isarranged before the first fractionation step, typ-ically after the last compression stage. Beforefeeding the compressor effluent to the molecularsieve dryer it is cooled in a water cooler and sub-sequently by propene refrigerant. A temperatureof 15 ◦C upstream of the dryer is desirable forremoving as much water as possible to reduceload on the dryers. However, the temperaturemust remain above the hydrate-formation point,which lies in the range 10 – 15 ◦C [50], [60].Wa-ter is adsorbed on molecular sieves, preferablyafter the highest compressionpressure is reachedto minimize adsorption costs. Higher pressureallows smaller dryer volume with lower adsor-bent cost and less water removal because thewater content in the gas stream decreases withincreasing pressure. Multiple adsorption bedsmake continuous water removal possible. Oneor more adsorption beds are in operation whileat least one unit is being regenerated. Regenera-tion requires the use of heated gas that is free ofpolymerizable components. Byproduct methaneand hydrogen used as fuel are typically goodchoices for this gas [50–53], [60], [61]. In liq-uid-feedstock cracking processes large amountsof hydrocarbons are condensed at 15 ◦C. If theseliquid hydrocarbons are to be fed to the fraction-ation column they are also dried over molecularsieve adsorbers.

5.3.2.2. Hydrocarbon Fractionation Section

The fractionation section receives the com-pressed cracked gas at a pressure of3200 – 3800 kPa for further fractionation intodifferent products and fractions at specifiedqualities and battery limit conditions. Over thehistory of design and construction of ethylene

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plants many different process schemes havebeen developed and implemented for this task.

Today, three processing routes have gainedcommercial importance, with the main charac-teristics being the first separation step and theposition of the hydrogenation of the acetylenecontained in the cracked gas. These three pro-cess sequences are:

1) Demethanizer first with tail-end hydrogen-ation

2) Deethanizer first with front-end hydrogen-ation

3) Depropanizer first with front-end hydrogen-ation

These basic processes differ in the configura-tion of process steps for any given feedstock,but provide similar overall capabilities for frac-tionation andhydrogenation. The differences areprimarily in the sequence of fractionation andhydrotreating steps downstream of cracked-gascompression [50].

Process Description. Compressed crackedgas can be:

1) Condensed and fed to a demethanizer col-umn (front-end demethanizer), as shown inFigure 24

2) Condensed and fed to a deethanizer (front-end deethanizer), as shown in Figure 25

3) Removed from an intermediate compres-sor stage, condensed, and depropanized ina column, whereby the light gas is returnedto the last compressor stage (front-end de-propanizer), as shown in Figure 26

Combinations are possible; for example, inter-mediate compressor stage condensate and vaporare sent to different parts of the plant [60], [56].

Traditionally the demethanizer first/tail-endhydrogenation process sequence was used byAmerican contractors. With the need for reduc-tion of energy consumption in the separationsection and process simplification for cost rea-sons, the deethanizer first/front-end hydrogen-ation process, which had long been used byLinde, was also applied by some American con-tractors. A comparison of all routes has shownthat this sequence seems to have the best en-ergy efficiency [63]. New developments in thisarea are the combination of the advantageous

sequence with special equipment (dephlegma-tors) [64] and the application of washing stepsfor demethanization [65].

Front-End Demethanizer (Fig. 24). Thehydrocarbon-separation sequence begins withremoval ofmethane and lighter components, pri-marily hydrogen, from higher molecular masscomponents. Hydrogen may be removed beforeor aftermethane. The bottomproduct is routed toa deethanizer column where acetylene, ethane,and ethylene are removed as overhead prod-uct, and C3 and heavier components as bottomproduct.

Typically, the overhead product from thedeethanizer is first hydrotreated to convert acety-lene to ethylene and ethane. This treated over-head mixture is then fractionated to ethyleneproduct and ethane recycle.

The bottom product from the deethanizer isdepropanized to separate C4 and heavier com-ponents as a bottom stream; methylacetylene,propadiene, propane, and propene are taken asan overhead stream. This overhead fraction ishydrogenated to remove methylacetylene andpropadiene, which can also be recovered bydistillation or absorption and stripping. In thepropene fractionation step, propene is recoveredfor sale and propane for recycle. The propeneproduct can be of chemical grade or polymergradewith additional purification. Depropanizerbottoms are sent to a debutanizer for separationinto other product streams (C4 materials, rawpyrolysis gasoline, C5 materials, aromatics, etc.)[50], [52–54], [59], [60].

Front-End Deethanizer (Fig. 25). Deeth-anization of dried cracked gas is used as thefirst fractionation step to produce on overheadstream of ethane and lighter components, anda product stream of C3 and heavier materials;subsequently, the lighter components are hydro-genated to remove acetylene and fractionatedcryogenically. Because this overhead stream ishydrogen rich, no supplementation is neces-sary for hydrogenation. During the chilling anddemethanizer operation, the overhead is sepa-rated into hydrogen and methane; the bottomstream is fractionated to yield ethylene prod-uct and ethane; and the ethane is recycled to thecracking furnaces.

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Figure 24. Simplified process flow diagram for the production of ethylene by liquid cracking with a front-end demethanizer

The bottom stream from the deethanizer isfed to the depropanizer. The overhead streamfrom the depropanizer is hydrogenated to con-vert methylacetylene and propadiene contami-nants to propene and propane. The final purifi-cation step yields propene product and propane;the propane is recycled as cracking feedstock.The depropanizer bottom stream is fractionatedto produce a C4 product stream and a C5-richraw pyrolysis gasoline [53], [54], [59], [60].

Front-End Depropanizer (Fig. 26). De-propanization of dried cracked gas is used asthe first fractionation step to produce a pro-pane and lighter component overhead streamand a C4 and heavier bottom stream. The de-propanizer overhead stream is compressed andhydrogenated to remove acetylene, and to par-tially hydrogenatemethylacetylene andpropadi-ene. It is then chilled and demethanized, and thebottom fraction is deethanized. The deethanizeroverhead components are fractionated to ethyl-ene product and ethane, which is recycled ascracking feedstock. Deethanizer bottom productis hydrotreated to remove methylacetylene andpropadiene, and fractionated to propene productand propane, which is recycled to the crackingfurnaces. The depropanizer bottom components

are fractionated to produce C4 materials and rawpyrolysis gasoline [53], [54], [59], [60].

For all three of the above-mentioned basicprocesses numerous process variants exist. Forliquid cracking acetylene hydrogenation is al-ways performed in the C2 stream, in the C2−or in the C3− stream. In the case of crackinggaseous feedstock with little co-production ofC4 hydrocarbons the hydrogenation step canalso be arranged in the total cracked gas streamduring or just after cracked-gas compression (af-ter or before drying). This is not feasible forcracked gas streams resulting from liquid crack-ing as 1,3-butadiene, typically a valuable by-product, would be cohydrogenated almost com-pletely to butene and butane.

Acetylene may also be recovered for sale byan absorption process. This absorption processstep is located in the gas phase upstream of theethylene fractionation column.

Prefractionation Feed Chilling. Before be-ing fed to any of the fractionation towers, driedcracked gas must be cooled and partially con-densed.Dried crackedgas is cooledby the refrig-erant systems and by the low-temperature prod-uct and recycle streams leaving the cold frac-tionation equipment down to a temperature of

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Figure 25. Simplified process flow diagram for the production of ethylene by liquid cracking with a front-end deethanizer

Figure 26. Simplified process flow diagram for the production of ethylene by liquid cracking with a front-end depropanizer

typically −140 to −160 ◦C. At this temperatureC2 components are entirely removed by partialcondensation, and the noncondensed gas streamhas a hydrogen concentration of 80 – 95 vol %.The type of refrigerant, number of refrigerationlevels, and the design of the refrigeration andheat-exchange systems depend on the temper-ature and pressure required in the downstream

fractionation equipment. Fractionation and pu-rification consume much energy. Cryogenic pu-rification of methane, ethane, and ethylene re-quires costly refrigeration. Design optimizationis complex because:

1) The most efficient routing must be consid-ered for the condensates and vapor streamsfrom each stage of the cool-down sequence

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in the individual refrigeration loops (e.g.,2 – 6 stages each)

2) The energy requirements for fractionationmust be determined

3) The freezing of components, such as acety-lene, butadiene, and benzene, must beavoided

When acetylene content is high, prevention offreezing and safe hydrogenation are important.Also of importance from a safety standpoint forthe chilling section and downstream equipmentis the choice of appropriate construction materi-als for cryogenic conditions [50], [52]. Processequipment that may accidentally be exposed tocryogenic conditions should also be carefullystudied. National standards are available in mostcountries to assist in making appropriate selec-tions [50], [52].

Demethanization. Demethanization ofcracked gas separates methane as an overheadcomponent from C2 and heavier bottom compo-nents; concurrently, hydrogen is removed fromthe cracked-gas stream andmay be obtained as aproduct by purification before or after demetha-nization. Methane is typically used as plant fuelor sold; C2 and heavier components are sentto the recovery system. This overall fractiona-tion is important from a design and operationalstandpoint because of its high share of the capi-tal, energy, and fuel consumption of the ethyleneplant. Demethanization typically consumes thegreatest proportion of net energy from the re-frigeration system (see Fig. 27 and discussionof refrigeration, page 44) [55], [62].

The feed stream to the demethanizer mustbe free of carbon dioxide and water to pre-vent freezing and plugging under the cryogenicconditions employed. Although a wide rangeof operating conditions is possible, feed tem-perature is typically ca. −100 ◦C and pressure3000 – 3500 kPa. Energy efficiency may be im-proved, often with increased capital cost andprocess complexity, by staged condensation andflashing of the stream during chilling to pro-vide multiple feed streams. Reboiling and con-densation at intermediate levels in the demetha-nizer, and lower dual-pressure demethanizationcan also be used. A range of gas compositionsmust be considered in the design [50], [53], [54],[59], [61].

The overhead condenser product contains hy-drogen, carbon monoxide, and small amountsof ethylene, in addition to methane. Inthe simplest case, expansion of the mixedmethane – hydrogen stream provides additionalrefrigeration, and the total gas effluent is used asfuel without refinement. Typically, however, af-ter condensation, some of the overhead methanefraction is flashed to about the pressure of fuelgas to obtain additional refrigeration. Any con-densate formed during this operation is a re-coverable source of ethylene. Additional stagedcooling equipment provides hydrogen of ca.95 vol % purity by adsorption processes. Thelower temperature refrigerant required in thisoperation is provided by expansion of the con-densed methane stream [50], [52], [55], [60],[61].

Energy is recovered from the demethanizeroverhead stream by Joule – Thompson pressurereduction or by an expansion turbine. The latter,in addition to generating refrigeration, recoverssome energy [57], [61].

The demethanizer bottom stream containsC2 and heavier components. With the front-end demethanizer, components fromC2 throughpyrolysis gasoline may be present. However,with front-end deethanization, C3+ compo-nents are removed, and with front-end de-propanization, C4+ components are removed.The demethanizer design changes significantlyas heavier components are eliminated, espe-cially with regard to the refrigeration needed tocondense the incoming cracked-gas feed streamand to reboil the bottom stream.

Deethanization. Deethanization of crackedgas separates acetylene, ethylene, and ethane asoverhead components from C3+ bottom com-ponents. In newer plants, low-pressure fraction-ation may be used, or feed streams from thecracked-gas chilling section can be supplied asmultiple feeds to the deethanization tower. Thedeethanizer is usually the third largest user ofrefrigeration energy in a front-end demethanizerethylene plant (Fig. 27) [50], [60], [61], [62].

With front-end demethanization and front-end depropanization, the feed stream to thedeethanizer comes primarily from the demetha-nizer. With front-end deethanization, the deeth-anizer feed comes from the chillers that followthe gas dryers. In the simplest cases, single feed

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streams from these units are separated into over-head and bottom fractions for further process-ing. More recent plant designs incorporate en-ergy savings into plant operation by providingan additional feed stream to the deethanizer fromthe feed-chilling section, along with that fromthe demethanizer [50]. Dual-pressure deetha-nizer systems improve energy consumption andreduce the bottom temperature, thus reducingfouling in reboilers. As with the demethanizer,these designs conserve refrigeration energy butincrease capital costs and operating complexity.The overhead product condensation temperatureis typically ca. 0 to −10 ◦C, based on a columnoperatingpressure of 1500 – 2700 kPa [53], [54],[59].

Depropanization. of cracked gas separatespropane and lighter fractions as overhead com-ponents from C4+ fractions as bottom com-ponents. Feed streams from compression, andsometimes streams from the gas-chilling sec-tion, can be routed to the depropanizer, which,compared to other fractionation units, requiresless refrigeration because of its higher operatingtemperature (Fig. 27) [62].

The feed stream to the depropanizer comesprimarily from the deethanizer when front-enddemethanization and deethanization are em-ployed. With front-end depropanization, thefeedstock is taken from the gas dryers. In thesimplest case, the dried cracked-gas feed streamis separated into a propene – propane overheadstream, which contains small amounts ofmethy-lacetylene and propadiene, and a bottom streamwhich contains components from C4 materialsto raw pyrolysis gasoline. Recent designs re-duce energy requirements by mixing smallerfeed streams removed from intermediate com-pression or gas-chilling stages with the mainfeed stream, or by having them enter separatelyat a point in the depropanizer consistent withthe composition of column components. Con-densate is usually stripped before entry into thedepropanizer [50], [61].

Operating pressure and temperature of thedepropanization step in ethylene plants, evendownstream of the deethanizer, are kept low toreduce fouling of the fractionator by acetylenicand diolefinic contaminants. Hydrogenation ofcracked gas in the compressor zone lowersthe amount of these polymerizing contaminants

substantially, but also destroys most of the buta-diene [50], [54], [59].

Debutanization. Debutanization of crackedgas separates C4 materials as overhead com-ponents from C5 and heavier fractions as bot-tom components. The feed stream comes typi-cally from the depropanizer column or is a de-propanized condensate stream from the com-pressor. The mixed C4 overhead fraction maybe sent to an extraction unit for removal of 1,3-butadiene and further processing. The bottomstream and the debutanized fraction from thecompression section can be used as pyrolysisgasoline feedstock or processed to produce aro-matics and specialty chemicals feedstocks [50].

Acetylene Hydrogenation. Cracked gas isselectively hydrogenated to facilitate removalof acetylene from ethylene, except when acety-lene is recovered for sale. Hydrogenation is per-formedwith palladium-based catalysts. Pressureranges typically from 20 to 35 bar and the tem-perature from 25 to 100 ◦C. There are two basicprocesses for the hydrogenation of acetylene.

Tail-End Hydrogenation. Acetylene hydro-genation takes place in the gas phase of a pureC2 fraction, consisting of ethylene, ethane, andacetylene only. The unit is typically incorporatedafter demethanization, upstream of the C2 frac-tionation tower. Hydrogenation reactors consistof one or two adiabatic beds. Hydrogen is addedupstream of the reactor at a molar H2/C2H2 ra-tio of ca. 1.5 – 2, resulting in an ethylene gain ofup to 50 % of the acetylene present. Hydrogenand small amounts of methane and CO intro-duced after demethanization must be removedby additional fractionation. Sometimes purgingthe light ends from the overhead ethylene frac-tionator condensate is possible, but additionalmultistage fractionation is usually required inthe ethylene fractionator or in a small separatedemethanizer. A useful design provides five toten overhead stages above the product drawoffpoint in the ethylene fractionator column for fur-ther separation of the light ends. The overheadcondensate is returned to the top of the tower,and the light ends are removed from the over-head partial condenser for reprocessing [50],[55], [60][62].

Front-End Hydrogenation. Acetylene is hy-drogenated:

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1) In the total cracked gas stream after or beforedrying

2) In the C3− stream with front-end de-propanizer

3) In theC2− streamwith front-end deethanizer

In the case of (1) and (2) any methylacetylene,propadiene and butadiene, present in the gasstream is cohydrogenated. (methylacetylene ca.80 %, propadiene 30 %, butadiene > 90 %).

Although hydrogenation in the compressorsection (1) may offer advantages for the lighterfeedstocks, disadvantages exist with heavierfeedstocks. In particular, the volume of gastreated at this stage is high; butadiene is hy-drogenated and lost; and a single hydrogen-ation to concurrently remove acetylene, methy-lacetylene, and propadiene to the required lev-els without significant olefin loss is not possible.Hydrogenation of individual mixed C2 and C3streams after deethanization and depropaniza-tion, respectively, appears to permit more effi-cient use of catalyst and result in higher prod-uct yields. However, proponents of the front-end deethanization and depropanization processwith front-end acetylene hydrogenation reportthat bed sizes are equivalent for that reaction.Higher hydrogen concentration and improvedcatalysts allow higher gas space velocities thancan be achieved downstream [60].

General advantages of the front-end hydro-genation versus the tail-end hydrogenation unitare: (1) no hydrogen make up is required as hy-drogen is already present in the feed stream;(2) longer run length between catalyst regener-ations; (3) No removal of light ends, as requiredin tail-end hydrogenation, is necessary.

Front-end hydrogenation is typically con-ducted in multistage adiabatic beds with in-tercooling, or less frequently in a singletubular reactor that allows a more isother-mal reaction. Acetylene hydrogenation re-quires heat-exchange systems for incoming low-temperature process streams (2) and (3). Hy-drogenation in the compressor section (1) doesnot require the heat-exchange system neces-sary for cryogenic streams. Most of the trouble-some polymerizable components are removedbefore fractionation, although rapid fouling ofthe hydrogenation bed must be avoided. Hy-drogenation may be necessary before chillingif a high acetylene concentration in the cracked

gas would result in plugging or in unsafe down-stream operation [50], [52], [60].

Although tail-end hydrogenation is the mostcommon process in currently operating plants, itseems that there is a strong tendency to increas-ingly apply the front-end hydrogenation systemin new projects.

Acetylene, Methylacetylene, and Propadi-ene Recovery. Acetylene,methylacetylene, andpropadiene may be recovered for use in weld-ing and cutting or as chemical feedstock. Acety-lene is usually extracted from the feed streamto the ethylene splitter, with methylacetyleneand propadiene coming from the overhead de-propanizer stream. Alternatively these materialsmay be extracted or distilled from the products;N-methyl-2-pyrrolidone, acetone, and N,N-di-methylformamide processes are typical recov-ery methods [50], [53], [60].

Ethylene Fractionation. Ethylene fraction-ation separates ethylene as a high-purity over-head product (> 99.9 wt%) from ethane, whichis combined with propane and recycled forcracking. For this difficult fractionation, the network done by the refrigeration system is highbecause of the high reflux and low temperaturerequired (Fig. 27) [50], [62]. Fractionation re-quires a high reflux ratio (ca. 4) and as manyas 125 separation stages [53], [54], [59], [60],[62]. The ethylene purity desired is typically> 99.9wt%. The feed stream comes from theacetylene-removal step that follows chilling, orfrom the demethanizer or deethanizer.

There are basically two processes in commer-cial use: high-pressure fractionation and heat-pumped C2 fractionation.

High-Pressure Fractionation. High-pressure fractionation, operating in the pres-sure range of 1700 – 2800 kPa, is typicallyused in tail-end hydrogenation systems. Heat-ing and cooling of the column is integratedinto the propene refrigeration cycle. Low-pres-sure propene refrigerant is vaporized in the topcondenser, providing chilling duty. Vaporizedpropene is typically compressed in two stages ofthe refrigerant compressor. After compression,propene vapors are condensed in the reboiler,providing heat duty. Bymeans of this system thepropene refrigerant compressor acts as a indirectheat pump, shifting heat from the condenser of

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the column to the reboiler. The top of the col-umn is equipped with some pasteurization traysto remove light ends introduced when acetyleneis hydrogenated in the feed stream to this col-umn. Ethylene product is withdrawn as a liquidside stream some trays below the top, pumpedto the required product pressure, and deliveredto battery limits after vaporization and heating.

Heat-Pumped C2 Fractionation. In heat-pumped C2 fractionation, the column operatesat a pressure of ca. 800 kPa. Overhead gases ofthe column, consisting of on-spec ethylene, arerouted to a compressor after heating to ambi-ent temperature in a feed – effluent exchangerand are compressed to ca. 2000 kPa. Part of thecompressed ethylene vapor is cooled and routedto the reboiler where it is condensed, providingheat duty for reboiling. The condensed ethyleneis recycled as reflux to the top of the column.Ethylene product is discharged to battery lim-its from the discharge side of the compressor.Heat-pumped ethylene fractionation can use adedicated compressor. More common is the in-tegration of the heat-pumped ethylene splitter inthe ethylene fractionation compressor, using the3rd stage of this compressor as a heat pump.

This process has some advantages over thehigh-pressure fractionation process with respectto investment and energy consumption. Lessequipment is involved, and because of the bet-ter relative volatility of ethylene and ethane atlower pressure, a lower reflux ratio is required.However it is not feasible to use the heat-pumpedprocess in combination with tail-end hydrogen-ation because of the light ends present in the feedstream.

Ethylene is generally discharged to batterylimits as a gas. However, production of up to50 % of production as the liquid phase and theuse of storage facilities is also practiced.

Hydrogenation of Methylacetylene andPropadiene (MAPD); C4 Fraction; and Py-rolysis Gasoline.

C3 Hydrogenation. The C3 fraction comingfrom the top of the depropanizer typically con-tains 2 – 6 % of methylacetylene (MA) andpropadiene (PD). For removal of these com-ponents from the propene product and foreconomic reasons MAPD is hydrogenated topropene and propane. Hydrogenation is per-formed in multistage adiabatic bed reactors with

intercooling steps or, in more modern processes,in a trickle-bed reactor. The heat of reaction is re-moved in the trickle-bed reactor by partial vapor-ization of the processed liquid, this being con-densed later by cooling water. Modern hydro-genation processes typically yield a net propenegain of 60 % of the MAPD present in the feedstream. The balance is converted to propane,which is recycled to the cracking furnaces ascracker feedstock.

C4 Hydrogenation. The C4 cut from the topof the debutanizer typically contains smallamounts of vinylacetylene and ethylacetylene,ca. 50 % 1,3-butadiene, and a few per cent ofbutanes; the balance consists of various types ofbutenes, of which isobutene is the most impor-tant. Depending on the nature of the downstreamprocesses it may be necessary to hydrogenatesome of the unsaturated components. The fol-lowing hydrogenation steps are in commercialuse:

1) Selective hydrogenation of butatriene andvinylacetylene to butadiene

2) Selective hydrogenation of butadiene tobutenes

3) Full hydrogenation of all unsaturated to bu-tane

Process (1) is applied to increase the 1,3 bu-tadiene yield; process (2) is used if no use canbe made of butadiene and to increase the buteneyield; process (3) is employed if the C4 cut isto be recycled as cracker feedstock to improveolefin yields or used as LPG product. Hydro-genation is performed in tubular reactor sys-tems or, in more modern processes, in trickle-bed reactor systems. By selecting catalyst typeand process parameters, the hydrogenation re-sult with respect to yields of different compo-nents, mainly the various types of butenes, canbe controlled in a certain range.

Pyrolysis Gasoline Hydrogenation. Pyroly-sis gasoline – the C5 to C10 hydrocarbon prod-uct fraction – consists mainly of aromatics. Thenonaromatics are mainly unsaturated hydro-carbons with a high portion of acetylenes anddienes. This stream is unstable and cannot bestored, as the unsaturated components react fur-ther, forming polymers and gum. Depending onthe downstream processes pyrolysis gasoline ishydrogenated and fractionated in different steps.The most common process route is as follows:

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1) Selective hydrogenation of the total gaso-line to hydrogenate acetylenes, dienes, andstyrene to olefinic compounds. After stabi-lization and removal of oil this stream is suit-able for use as motor fuel.

2) Fractionation of the effluent of the 1st stagehydrogenation into a C5 cut, a C6 –C8 heartcut, and a C9+ cut.

3) The C6 –C8 cut is further processed in a 2ndstage hydrogenation step to convert olefinsto paraffins and naphthenes and to convertall sulfur to H2S, which is removed from theproduct in a downstream stripper. this pro-cess is necessary to prepare the heart cut foraromatics recovery.

Propene fractionation separates propene asa chemical-grade overhead product (typically93 – 95 wt% min.) or more frequently aspolymer-grade propene (> 99.5 wt%) from pro-pane. This separation to polymer grade propenerequires typically 150 – 230 stages and a re-flux ratio of 20 because of the close boilingpoints of propene and propane. Two basic pro-cesses are applied for this difficult separationtask: polymer-grade fractionators operate at ca1800 kPa, with cooling water in the overheadcondenser and hot quench water in the reboiler.In the case of naphtha cracking and where suf-ficient waste heat is available from the hotquench water cycle this is the most economicprocess. If no waste heat for reboiling is avail-able, a heat-pumped propylene fractionator isapplied. In this case the fractionator operatesat ca. 800 – 1100 kPa, and the overhead gasesare compressed and condensed in the reboiler.By means of this process the condenser heat israised to a higher temperature level, and furtheruse ismade of it in the reboiler. The advantage ofthis system is that no external heat for reboilingand only small quantities of cooling water arerequired. The fractionation design depends onthe concentration of propene in the feed, whichvaries from 70 % for propane cracking to 95 %for naphtha cracking [60–62].

The feed stream to the propene fractiona-tor usually comes from the methylacetylene andpropadiene removal step. Excess hydrogen andmethane are purged in an upstream stripper oras light ends in the column overhead or from theoverhead condensate [53], [54], [59–62].

Hydrogen Purification. Hydrogen is pro-duced in the cryogenic section of the plant ata purity of typically 80 – 95 vol%. However, theproduct stream contains some 1000 ppm of car-bon monoxide. Hydrogen product is required inthe ethylene plant as make-up stream for the hy-drogenation units. Excess hydrogen is typicallya desired product. However, hydrogen must befree of carbonmonoxide as CO is a poison for allhydrogenation processes. Today two processesare in commercial use in ethylene plants to pu-rify hydrogen: (1) methanation of CO in a cat-alytic process, converting CO to methane andwater, after which the effluent must be driedin adsorber beds; (2) hydrogen purification byadsorption in a pressure-swing adsorption unit,producing CO-free high-purity hydrogen.

5.3.3. Utilities

Refrigeration. Refrigeration in ethyleneplants is important and costly. Refrigeration op-timization is vital in plant design. Typically, twodifferent refrigeration systems are employed,namely, ethylene and propene (or propene – pro-pane), each of which generates two to five dif-ferent temperatures. Propylene refrigeration isdesigned as a closed-loop system in which theheat removed by cooling water or by air cool-ing by condensing the refrigerant after the finalcompression stage. Ethylene refrigeration sys-tems are designed as closed- and open-loop sys-tems. Open-loop cycles integrate the ethylene-fractionation tower in the refrigeration system.Propane and ethylene refrigerant systems actas a chilling cascade. Heat removed from theprocess by the ethylene cycle at temperaturesbelow −50 ◦C is shifted to the propene cycle bycondensing high-pressure ethylene refrigerantby means of vaporizing low-pressure ethylenerefrigerant. Refrigerant temperatures are cho-sen to accommodate diverse plant needs mostefficiently. Methane refrigeration by simple ex-pansion (not employed as a refrigeration loop)generates additional cooling and especially thelower temperatures needed to purify hydro-gen for special purposes. Ethylene, propene,and propane are used because of their physicalproperties and availability in the ethylene plant[61].

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Figure 27 shows the most common refriger-ant loops and the net heat and work required ina typical front-end demethanization plant withliquid feedstock. The less expensive refriger-ant, propene, is used from + 25 to − 40 ◦C andthe more expensive ethylene, from ca. −40 to− 100 C The latter requires higher work inputper unit of refrigeration;for example, Figure 27shows that 41 % of the heat absorbed by the eth-ylene refrigeration system requires 58 % of thenet work [62]. Refrigerants are usually gener-ated by compression to 1600 – 2000 kPa in mul-tistage units, followed by expansion to gener-ate the lowest refrigeration temperature. Super-heated ethylene is cooled and condensed withpropene refrigerant. Propene, after compression,is cooled with process cooling water [53], [60],[62]. With open-loop systems, which are usedless frequently, products are circulated in therefrigeration loops rather than isolated. Care-ful operation and reliable design of compressors(gas seals) reduces contamination [60].

Energy. Utility consumption, expressed injoules per kilogram, is the energy required toproduce 1 kg of ethylene product. Feedstock,coproducts, and process design should be de-scribed fully for comparative purposes. Processoptimization has to consider the cost of energyrelative to capital costs, ease of process opera-tion, product and byproduct quality control re-quirements, safety, andmany other issues. Sincethe early 1970s until today, increased energycosts led to a reduction of energy consumptionby nearly 50%. This was accomplished by usingprocess water heat, side reboilers, heat pumps,and other devices.

Approximate energy consumption to produce1 kg of ethylene from various feedstocks is asfollows:

Ethane 14 300 J/kgPropane 16 700 J/kgNaphtha 20 900 J/kgGas oil 25 100 J/kg

These values are approximate because flowschemes and product distribution are undefined,but they are representative. A reduction of ca.2000 J/kg ethylene product is possible by us-ing hot exhaust from gas turbines in the pyro-lysis area as combustion air to preheat combus-tion fuel, or in a heat-recovery boiler. The tur-

bines may also optimize energy use to produceelectricity or can drive fractionation compres-sors and heat pumps [50], [52], [57], [58], [60],[61], [62].

Most of the energy consumed is introducedinto the ethylene process via firing the crack-ing furnaces. The recovery process is driven bywaste heat, recovered from the cracking furnacesvia steam production in the TLEs or by recov-ering heat from the furnace effluent stream. Themain energy consumers in the recovery sectionare the cracked-gas compressor and the refrig-erant compressors, in which a total power of ca.0.7 kWh per kilogram ethylene is typically con-sumed. This power is usually provided by steamturbines, driven by steam generated and super-heated in the cracking furnaces.

5.3.4. Process Advances

Major advances have been made in feedstockavailability and process design [50], [62]:

– Feedstock cost and availability, new crack-ing technology, and concerns for the envi-ronment and health have influenced changesin process technology.

– Rapid development has occurred in processcontrol, data management, and optimizationsystems. Control of individual units, as wellas of the overall process, has had a signifi-cant impact on operations. Improved analy-sis and cracking-simulation models are re-quired to more fully apply state-of-the-artprocess control.

– Major improvements have been made in theselectivity and efficiency of cracking by op-erating at higher temperature. Coils withshorter residence time and faster quenchingsystems have been developed. Energy re-quirements have been reduced by heat re-covery from furnace flue gas, economizergas, and cracked gas; refrigeration energy re-quirements have been lowered by increasedapplication and improved design of heat-exchange and distillation systems.Use of gasturbines has increased, with the sale of elec-tricity generated. At the same time, control,reliability, and efficiency of operation haveimproved [60], [61].

– The reliability, service life, and cost of solid-desiccant drying systems have improved.

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Figure 27. Distribution of heat load and work requirement of the refrigeration system in a typical front-end demethanizerethylene plant ∗A) Distribution of heat load and work requirementa) Net heat absorbed by the refrigeration system; b) Net work done by the refrigeration systemB) Relative cost of heat absorbed by the refrigeration system at different temperatures∗Reprinted with permission [62].

– Improved fractionation process designs pro-vide additional flexibility and further reduceprocess energy consumption while meet-ing plant-reliability and product-quality de-mands [61].

– Improved hydrogenation catalysts allowmore selective removal of impurities and bet-ter quality control.

5.4. Other Processes and Feedstocks

Ethylene has also been produced by other pro-cesses and from other feedstocks [66]. Optionsfor long-range feedstock availability and price,as well as in-place refining and chemical pro-cesses, influence process design and feedstockselection because of their high economic impacton manufacturing cost.

Recovery from FCC Offgas. Recovery ofethylene and propylene from FCC offgas hasgained importance, but due to the NOx content, some steps have to be integrated to reduce therisk of formation of explosive resins from buta-diene and N2O3.

Ethanol. Ethanol, an early ethylene feed-stock, is dehydrated at high temperature over asolid catalyst. The catalyst is usually supportedalumina, phosphoric acid, or silica. The etha-nol can be obtained from fermentation, meth-anol homologation, syngas and other sources(→Ethanol, Chap. 4. and →Ethanol, Chap. 5.).

Crude Oil or Residual Oil. A number ofnontubular reactors, developed to crack unpro-cessed hydrocarbon feedstocks, exist in variousstages of development and commercial opera-tion [66].

A new development by Stone &Webster em-ploys catalysts particles, for cracking and heattransfer functions. The QC (Quick Contact) pro-cess is suitable for cracking VGO and similarheavy feedstocks. The process has been testedin a pilot plant [67].

A new development by Veba Oil and Lindeemploys a catalyst with coke-gasification func-tions. This allowsheavy feedstocks such asAGOand VGO to be processed in a reformer-type re-actor to yield olefins. The high coking tendency

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of these feedstocks, which normally limits theiruse as feed for crackers, is no longer a problem,since the coke deposits are continuously gasified[68].

Other new developments use plastics wastesas feedstocks for olefins production. A pro-cess developed by BP produces a liquid feed-stock from waste plastics which is suitable ascracker feedstock [69]. Another development byLinde directly co-processes polyolefin wastes inamodified cracking furnace, giving better yieldsthan commercially cracked liquid feeds [70].

Methanol can be catalytically dehydratedand partially converted to ethylene over alu-mina and zeolite catalysts. The process basedon novel zeolite catalysts (ZSM-5) was devel-oped by Mobil (MTO, Methanol to Olefins).A new development introduced by UOP/NorskHydro, converts methane to methanol in a firststage and then converts the methanol to olefins.Economics of this new process seem to be com-petitive with conventional processes [71]. Theprocess is based on a fluidized-bed reactor forconversion of methanol. 80% of the carbon con-tent of methanol is converted into ethylene andpropylene. The process has been tested in 0.5 t/dunit in Norway. Methanol obtained from syngascan be converted in high selectivity (but at a lowrate) to ethanol with the help of catalysts andpromoters.

Syngas. Fischer – Tropsch and modifiedFischer – Tropsch processes are used to produce(1) olefins directly as a byproduct of gasolineand diesel fuel production; (2) LPG and paraf-fin intermediates, which are cracked to produceolefins; and (3) intermediate oxygenated liquids,which are dehydrated and separated to produceolefins (→Coal Liquefaction). Syngas is pro-duced by gasification of coal and other materials(→Gas Production).

Oxidative Coupling of Methane to Ethy-lene. Many researchers worldwide have beenactive in this field, using metal oxide catalystsat 700 – 900 ◦C for the oxidative coupling ofmethane. However, the yields obtained so far(20 – 25 %) are not competitive with conven-tional routes, since the ethylene concentration inthe product gas is only ca. 10 vol % [72], [73].

Application of special separative reactors has ledto improved yields up to 50 – 60 % [74], [75].

Dehydrogenation. Dehydrogenation ofethane over Cr or Pt catalyst is limited byequilibrium and allows only very poor yieldof ethylene. This route is not competitive withconventional routes.

Metathesis. Metathesis of propylene leadsethylene and 1-butene:

2C3H6−→←− C2H4 +C4H8

Since this reaction is reversible the ethyl-ene/propylene production of a plant can be ad-justed to market conditions. So far this technol-ogy is applied in a plant in Canada and at theU.S. gulf coast.

6. Environmental Protection

Ethylene plants with a production of up to900 000 t/a ethylene and a fired duty of up to700mW require special measures for protectionof the environment. Though national standardsvary widely, the following general measures arerequired for every new plant:

Flue-Gas Emissions. NOx emissions arelimited by use of LowNox burners or integratedSCR technology for catalytic reduction of NOx.In some regions limits for NOx emissions arealready < 50 ppm. Particulate emissions duringdecoking can be reduced by incineration or sep-aration in cyclones. Incinerators can achieve areduction of 90 %, and high-performance sepa-rators, up to 96 %.

Fugitive Emissions and VOC. The equip-ment used in a modern olefin plant has to meetthe standards for emission of critical compo-nents such as benzene. All components with apotential to emit critical components must havea certain tightness classification and have to bemonitored (pump seals, valves, etc.). Storagetanks and piping are other sources of fugitiveemissions

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Flaring. Flaring during start up should beavoided asmuch as possible, especially in highlypopulated areas. New procedures have been de-veloped that allow for flareless start up of plant[76].

Noise Protection. Ethylene plants containequipment that produces noise emission in therange above 85 dBA. These are the burners at thefurnaces and the large compressors.Noise abate-ment measures are essential (silencers for burn-ers, hoods for compressors) to bring the overallemissions into the range below 85 dBA. Othersources of noise emission can be high veloci-ties in piping or vibrations. The detection of thesource in this case is sometimes very difficultand requires much expertise.

Water Protection. The water emissions ofthe plant result from quench water, dilutionsteam, decoking water, and flare water dis-charges. These streams have to be treated prop-erly before being fed to the wastewater plant.Streams from the caustic-scrubbing section re-quire chemical treatment (oxidation) before dis-charge to the wastewater unit.

Solid and Hazardous Wastes. Examples ofprocess wastes are cleaning acids; filter car-tridges; catalysts; tars; polymers; waste oils;coke; sodium nitrite used in column passivation;N,N-dimethylformamide, acetone, or N-methyl-2-pyrrolidone used in acetylene removal; sulfu-ric acid from cooling towers; amine tars; andantifoaming agents. These wastes have to betreated according to the relevant regulations fordisposal.

7. Quality Specifications

Ethylene quality worldwide is matched to cus-tomer requirements; no single chemical-gradeethylene exists. However, ethylene content nor-mally exceeds 99.9wt%. The reason for varia-tion in ethylene specifications is due to the useof ethylene in downstream processes that dif-fer in sensitivity to impurities in ethylene, dueto different catalyst systems being used. In gen-eral, the trend is towards lower impurity contentsas more active catalyst systems are developed.

The largest application for ethylene is polymer-ization to HDPE, LDPE, and LLDPE. For theseprocesses new catalyst systems have been devel-oped, including themetallocene catalysts, whichare more sensitive than other catalysts. Table 11lists typical ethylene specifications for variouspolymerization processes.

Sulfur, oxygen, acetylene, hydrogen, carbonmonoxide and carbon dioxide are the most trou-blesome and carefully controlled impurities, es-pecially when ethylene from multiple sources ismixed in transportation.

8. Chemical Analysis

Laboratory analysis of ethylene is primarily byASTMormodified ASTMgas chromatographictechniques.

Process control may use over 100 analyzersto monitor plant safety, operation, and optimiza-tion [78]. Measurements include personnel ex-posure, corrosion, furnace flue gas, steam sys-tems, water systems, condensate systems, stackemissions, water emissions, feedstock quality,cracked gas analysis, distillation train productquality andmoisture control, and, in some cases,heavy liquids product evaluation and control[79].

Process control instruments include gas chro-matographs, combustible-gas detectors, conduc-tivity analyzers, pH meters, densitometers, cor-rosion analyzers, oxygen and water analyzers,vapor pressure analyzers, and photoionizationanalyzers. Various automated wet methods arealso used [78].

Process optimization is critical for ethyleneproduction because cracking reactions changeas the run proceeds. Operating costs for plantsof this size are high [51], [80], [81]. Advancesin computer control, data acquisition, and infor-mation analysis have given impetus to studiesof process control, modeling, and optimization,especially in heavier liquid cracking operations.

Models for all kinds of feedstocks are ap-plied, simulating all sections of the plant in de-tail, based on detailed chemical analysis of thevarious streams in the plant. With these toolsoperating strategies can be followed, e.g., pro-duction of a certain amount of ethylene, pro-pylene and other products at maximum profit,even if the feedstock quality or the type of feedchange within short time. Such a computer con-

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48 Ethylene

Table 11. Typical ethylene specifications (in ppm vol unless otherwise noted) [77]

Polymer Process

Component Gas phase Slurry Solution Matallocene a Polymer grade(today)

Ethylene 99.9 % min. 99.95 % min. 99.9 % min. 99.9 % 99.9 % min.Methane 500 b 500 b e 300Ethane 500 b 500 b e 500Propylene 20 20 50 20 10 – 15Acetylene 0.1 2 55 0.1 2Hydrogene 5 5 10 5 10Carbon monoxide 0.1 1 c 2 d 0.1 2Cabon dioxide 0.1 1 c 5 d 0.1 2Oxygen 0.1 1 5 0.1 5Water 0.1 5 c 5 d 0.1 2MeOH 1 c 5 d 0.1 5Sulfur as H2S 1 (wt) c 2 (wt) d 0.1 2 (wt)Other polar compounds 1 2 0.1DMF 2 (wt)

a Values for metallocene catalyst are expected values. b Total combined not to exceed 0.125 %. c Total not to exceed 1 ppm wt. d Totalmust be less than 6 ppm.e Total combined not to exceed 300 ppm wt.

trolled operation includes the individual controlof cracking furnaces, columns, pumps, compres-sors, etc.

9. Storage and Transportation

Much ofworld ethylene production is consumedlocally, requiring little storage and transporta-tion. Interconnected pipelines and pressurizedunderground caverns in the United States andEuropehavebeendevelopedbecauseof the com-plex petrochemical infrastructure. They provideflexibility and prevent interruption of supply.The following pipeline systems have been de-veloped:

United States: Texas – Louisiana [83]Canada: Fort Saskatchewan – Sarnia [82]Great Britain: Grangemouth –Carrington

Sevenside – Fawley [53]Europe: Northwest Europe

(Frankfurt –Gelsenkirchen andBrussels – Rotterdam areas) and Spain [53],[84], [85]

Former SovietUnion:

Nizhnekamsk – Salavat and Angarsk – Zima[86], [87]

In the U.S. Gulf Coast area the pipeline gridis composed of common carriers and privatelyowned pipelines. Storage caverns are naturallyoccurring or artificially excavated salt domes;limestone caverns are less usual. In contrast toU.S. pipelines, which normally transport onlyethylene, the 3000 km pipeline between Fort

Saskatchewan and Sarnia transports ethane, pro-pane, and condensate in batches [51], [82].

In pipelines, ethylene is normally under apressure of 4 – 100MPa. The upper end of thepressure range is significantly above the criticalpressure. Below critical conditions, the temper-ature must be > 4 ◦C to prevent liquid ethylenefrom forming. If water is present, hydrates canform below 15 ◦C at normal operating pressureand can plug equipment. Special procedures andprecautions are used during commissioning ofpipelines to pressure test and dry the line and toprovide appropriate draining and venting duringoperation [85].

Ethylene decomposition and spontaneous ig-nition can occur under certain conditions andcan result in pressure and temperature increasescapable of producing explosions. Such decom-position is a function of pressure, temperature,impurities (e.g., acetylene and oxygen), and cat-alysts (e.g., rust and carbon). Appropriate com-pression procedures, especially when nitrogen,oxygen, or other diatomic gases are present, helpto prevent decomposition [88].

Ethylene is also transported by ship, barge,railcar, and tank truck. In theUnited States, thesemethods are normally limited to consumers notserved by pipeline. In Europe, pipelines move alower proportion of ethylene than in the UnitedStates.

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Table 12. World consumption of ethylene in1993 (in %)

Use N. America W. Europe Japan Others Total

HDPE 24 20 18 26 23LDPE/LLDPE 29 37 31 35 33Dichloroethane 15 15 17 13 15Ethylbenzene 7 7 11 6 7Oligomers 5 3 ∗ 0 2Acetaldehyde 1 ∗ 4 1 2Ethanol ∗ 2 ∗ 1 2Vinyl acetate 2 1 3 1 2Other uses 3 6 6 2 3

Total 100 100 100 100 100

∗ Included in other uses.

Table 13. Regional supply (excluding standby capability) and demand estimates in 1993

Region Capacity, 106 t/a Production, 106 t/a Utilization, %

North America 24 948 22 834 92Western Europe 18 886 15 737 83Japan 6 776 5 773 85Others 24 534 17 905 73World 75 144 62 249 83

Ethylene is also stored in underground high-pressure pipelines and tanks (e.g., at 10MPa)and in surface refrigerated tanks. In the latter,compression and liquefaction of vapor from therefrigerated tank, followed by reinjection of theliquid, allow operation of the tank at pressuresof only 7 – 70 kPa [51], [89].

10. Uses and Economic Aspects

More than 80 % of the ethylene consumed in1993 was used to produce ethylene oxide; eth-ylene dichloride; and low-density, linear low-density, and high-density polyethylene. Signif-icant amounts are also used to make ethyl-benzene, oligomer products (e.g., alcohols andolefins), acetaldehyde, and vinyl acetate. LDPEand LLDPE are the fastest growing outlets forethylene.

Table 12 shows the uses of ethylene by regionfor 1993 [90].

By far the largest market for ethylene is theproduction of polymers. Polyethylene and PVCare projected to grow at rates of 5 %/a [90].Ethylene oxide and ethylbenzene are projectedto grow at rates of 4 and 4.5 %/a, respectively.In contrast, some derivatives such as ethanol and

acetaldehyde will continue to lose market sharesas a result of competing technologies.

The estimated 1996world nameplate produc-tion capacity and the actual consumption wereover 79.3× 106 t/a and 70× 106 t/a, respec-tively [2]. Regional supply (excluding standbycapability) and demand estimates are shown inTable 13. Conversion products of ethylene aregiven in Table 12 for the United States, West-ern Europe, Japan and for the world.

The principal influences on ethylene prod-uct value from the manufacturer’s viewpoint areprimarily the price of feedstock raw materials,chemical and byproduct credits, and expectedreturn on capital costs associated with the facili-ties. The fixed cost component for ethylene pro-duction is relatively modest because of the high-volume commodity operation that has becomethe industry standard (e.g., up to 950× 103 t/asingle-train plants). The cost breakdown pertonne of ethylene produced is listed below fora new plant based on naphtha feedstock in theAsia/Pacific region:

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50 Ethylene

Basis of economic analysisCapacity 500 000 t/aLocation Asia/PacificFeedstock naphthaCapital 10 years linear depreciation for

ISBL plant15 years linear depreciation forstorage

Investment cost estimate $ 420× 106for ISBL plant$ 80× 106 for OSBL plant

Cost breakdown, %/t ethylene producedFeedstock costs 47.4Catalysts and chemicals 0.5Utilities 0.3Cash cost 48.6Operating costs 1.9Overheads 1.9

11. Toxicology and OccupationalHealth [91]

Ethylene is not markedly toxic, but high con-centrationsmay cause drowsiness, unconscious-ness, or asphyxia because of oxygen displace-ment [92], [93]. The gas possesses useful anes-thetic properties, with rapid onset, quick recov-ery, and minimal effects on the heart or lungs[94].

In animal studies, ethylene was not irritatingto the skin or eyes [95]. It did not cause car-diac sensitization in a dog [96]. Mice and ratsexposed repeatedly to ethylene showed mini-mal effects [97], [98]. In a chronic inhalationstudy with rats, no toxic effects were found byhistopathology, hematology, clinical chemistry,urinalysis, eye examination, or mortality rate[98]. Ethylene improved wound healing follow-ing muscle injury to mice [99].

Studies with rodents have shown that eth-ylene caused increased serum pyruvate andliver weights [100], hypotension [101], de-creased cholinesterase activity [98], hypo-glycemia [102], and decreased inorganic phos-phates [95]. Nomutagenic activitywas observedin Escheria coli B and E. coli Sd-4 exposed toethylene [103].

Ethylene is a plant hormone and is use-ful for ripening fruits and vegetables [104],[105]. At high concentrations, it is phytotoxic[106]. Human exposure to ethylene is reportedto cause anorexia, weight loss, insomnia, irri-tability, polycythemia, nephritis, slowed reac-tion time, and memory disturbances [107–109].In the workplace, ethylene is treated as a sim-ple asphyxiant [110]; the odor threshold is ca.

20 ppm [111]. NIOSH has published a proce-dure for evaluating ethylene exposure [112].

As with any compressed gas, skin and eyecontact should be avoided. Appropriate precau-tions are required because the gas is highly flam-mable and explosive over a wide range of mix-tures with air. Ethylene is also spontaneouslyexplosive in sunlight in the presence of ozone orchlorine, and reacts vigorously with aluminumchloride and carbon tetrachloride [91].

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