Complete

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THE HISTORY OF MODERN PIPELINE EQUATION GROUP 2

Transcript of Complete

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THE HISTORY OF MODERN PIPELINE EQUATION

GROUP 2

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VISCOSITY EFFECT

ROUGHNESS OF PIPE WALL

FRICTION LOSSES

FRICTION LOSSES

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WALL SHEAR STRESS

KINETIC ENERGY PER UNIT VOLUME

FRICTION FACTOR

FRICTION FACTOR

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Fanning eq. Darcy-Weisbach Moody

FANNING, DARCY-WEISBACH,MOODY

f = 4f’

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• Ratio of fluid momentum forces to viscous shear forceDEFINITION

• Distinguish laminar and turbulent flowPURPOSE

THE REYNOLDS NUMBER, NRE

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BASIC EQ AND NATURAL GAS FLOW

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absolute roughness/

internal diameter

e/D

RELATIVE ROUGHNESS

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Hagen

Poiseuille

Moody

f = f(NRE, e/D)

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f = 64/NRE

LAMINAR SINGLE PHASE FLOW

!

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Smooth Wall Pipe

Rough Wall Pipe

! TURBULENT

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Gas Flow Equation

Weymouth Equation

Clinedinst EquationOliphant Equation

Panhandle’s Equation

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Panhandle’s Equati

on Panhandle A

Panhandle B

Develop in 1940s

Develop in 1956

• The friction factor is a function of

Reynold’s number.• Design for large diameter and long

pipelines.

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EQUATION OF PANHANDLE A

f varies with NRE

Pipeline Flow equation

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EQUATION OF PANHANDLE B

f varies with NRE

Pipeline Flow equation

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OLIPHANT EQUATION

1) Designed for low pressure gathering system

2) Extensively use for vacuum and low pressure (25-35 psig)

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0.

5

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WEYMOUTH EQUATION

Calculate the flow rate and pressure losses in

horizontal pipeline

w/o modifications, its being used for pipelines

operating in 35-100 psig

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Modified eq.

f varies with diameter

Original eq.

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No mechanical work steady flow isothermal flow constant compressibility factor horizontal flow no kinetic energy changes.

ASSUMPTIONS

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When discussing this topic, we will only consider Weymouth equation:

SERIES VS PARALLEL

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Consider an L-mile long, DA-in. internal diameter operating with total pressure drop of p1-p2.

SERIES

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The pipeline is altered by replacing the first LB miles with a DB-in. internal diameter line) and value of pressure drop, p1-p2 is constant.

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Using Weymouth equation, and since p1-p2 is constant, the equation can be written as:

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where K is a constant. The equivalent length of a DA-in. line, L’A that would have the same pressure drop as LB miles of DB – in. line is:

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Therefore, the series line shown have a total equivalent length of:

Percent of change in flow rate :

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The equivalent lengths and diameters can be expressed as:

If Weymouth equation with friction factor f is used, the equation will become:

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If there are more than 2 pipes in series, the equation will become:

In term of friction factor, f :

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Consider L-mile, DA-in. internal diameter. Suppose the full length is paralleled with new DB-in. internal diameter.

PARALLEL

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Old flow rate using only DA-in. line = qA . New flow rate with both lines is qt = qA + qb. The length, L is constant. Using Weymouth equation:

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The ratio of new to old flow rates is:

Pressure increase in capacity is:

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If the length of the two parallel lines is not equal, this equation shall be used:

The ratio of the flow rates becomes:

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Those equations may be extended to more than 2 lines in parallel. It will become:

In terms of friction factor,f:

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