DUG 48-860-1 Kurko - Consideration of Autocatalytic Behavior
Transcript of DUG 48-860-1 Kurko - Consideration of Autocatalytic Behavior
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Consideration of Autocatalytic BehaviorConsideration of Autocatalytic Behaviorin Determination of Self Acceleratingin Determination of Self Accelerating Decomposition TemperatureDecomposition TemperatureKenneth Kurko1, Charles Kozlowski1, Bertrand Roduit2
1Fauske & Associates, LLC, 16W070 83rd
Street, Burr Ridge, IL 60527, USA2AKTS AG Advanced Kinetics and Technology Solutions, TECHNOArk
1, 3960 Siders, Switzerland
Presented by Kenneth Kurko
to 2011 Fall DIERS User GroupOctober 12 2011
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What is a Self AcceleratingWhat is a Self Accelerating
Decomposition Temperature?Decomposition Temperature?United States SADT Test: SADT
is defined as the lowest
environmental temperature atwhich the center of the material
within the package heats to a
temperature 6C greater than
the environmental temperatureafter a lapse of a seven day
period or less. This period is
measured from the time whenthe temperature in the center of
the package reaches 2C below
the environmental temperature.
2Proprietary property of Fauske & Associates, LLC
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What is Needed to Estimate a SADT?What is Needed to Estimate a SADT?
Package properties
- Size
- Heat
transfer
coefficient
Physical
properties
of self-reactive
substance
- Density
- Specific
heat
- Thermal conductivity
Decomposition kinetics
3Proprietary property of Fauske & Associates, LLC
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AzodicarbonamideAzodicarbonamide (CAS: 123(CAS: 123--7777--3)3)
4Proprietary property of Fauske & Associates, LLC
Package properties
- Size (50 kg)
- Heat transfer coefficient (5 W/m2K)
Physical properties of self-reactive substance
- Density (1650 kg/m3)
- Specific heat (1050 J/kgK)- Thermal conductivity (0.1 W/mK)
Decomposition kinetics
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AzodicarbonamideAzodicarbonamide (CAS: 123(CAS: 123--7777--3)3)
Package properties
- Size (50 kg)
- Heat transfer coefficient (5 W/m2K)
Physical properties of self-reactive substance
- Density (1650 kg/m3)
- Specific heat (1050 J/kgK)- Thermal conductivity (0.1 W/mK)
Decomposition kinetics
5Proprietary property of Fauske & Associates, LLC
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Adiabatic Calorimetry
- ARC- VSP2
- ARSST
Heat Flow Calorimetry- TAM- C80
- DSC
Methods of Investigating Decomposition ReactionsMethods of Investigating Decomposition Reactions
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Methods of Investigating Decomposition ReactionsMethods of Investigating Decomposition Reactions
Adiabatic Calorimetry
- ARC- VSP2
- ARSST
Heat Flow Calorimetry- TAM- C80
- DSC
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NonNon--Isothermal DSC SignalsIsothermal DSC Signals
Temperature (C)
200180160140120
HeatFlow(W/g)
8
6
4
2
0
0.25C/min
0.5C/min
1C/min
2C/min
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Isothermal DSC SignalsIsothermal DSC Signals
Time (h)
65.554.543.532.521.510.50
HeatFlow(W/g)
0.35
0.3
0.25
0.2
0.15
0.1
0.05
0
-0.05
-0.1
170C
165C
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Basic Kinetic EquationBasic Kinetic Equation
Reaction rate is expressed by the equation
- Where A, E, f(), T, and t mean: pre-exponential factor in Arrheniusequation, activation energy, function of the reaction extent
which
form depends on the decomposition mechanism, temperature, andtime, respectively
Isoconversional methods (model free)
- Reaction model is not required
f
tTR
EexpA
dt
d
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Isoconversional MethodsIsoconversional Methods
Reactionrate
expressed
by
the
Arrhenius
equation
Reactionrateatagivenreactionprogress
isonlyafunctionofthetemperature
A()andE()arethepreexponentialfactorandapparentactivationenergy
Isoconversional methods (model free)
- Three main modifications of isoconversional method are applied in the
literature Differential (Friedman)
Integral (Flynn-Ozawa-Wall)
ASTM E698
T
1
R
E)(A'ln
dt
dln
=
fA
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Reaction Progress Under Isothermal (A)Reaction Progress Under Isothermal (A)
& Non& Non--Isothermal (B) ConditionsIsothermal (B) Conditions
Time (h)
4.543.532.521.510.50
Reactionprogress(-)
1
0.8
0.6
0.4
0.2
0
170C 165C
Temperature (C)
205200195190185180175170165160155150145
Reac
tionprogress(-)
1
0.8
0.6
0.4
0.2
0
0.25C/min 0.5C/min 1C/min 2C/min
rHQ
(A)
(B)
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Reaction Rate Under Isothermal (A)Reaction Rate Under Isothermal (A)
& Non& Non--Isothermal (B) ConditionsIsothermal (B) Conditions
Time (h)
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Rea
ctionrate(-/s)
2.5E-4
2E-4
1.5E-4
1E-4
5E-5
0
170C
165C
Temperature (C)
205200195190185180175170165160155150145
Reactionrate(-/s)
0.007
0.006
0.005
0.004
0.003
0.002
0.001
0
0.25C/min
0.5C/min
1C/min
2C/min
rH
Q
dt
d
(A)
(B)
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Differential Isoconversional MethodDifferential Isoconversional Method
1000/T (1000/K)
2.352.32.252.22.152.12.05
ln(Reactionrate(-/s))(-)
-4
-6
-8
-10
-12
-14
0.01
0.02
0.050.1
0.7
0.8
0.9
0.95
0.98
0.99
The activation energy is determined from the slope of the lines,
connecting points plotted incoordinates: reaction rate vs. 1/T, obtained for the same reaction progress
at different
heating rates
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Dependence of EDependence of Eaa
& ln(A) on& ln(A) on
the Reaction Progressthe Reaction Progress
Reaction progress alpha (-)
10.80.60.40.20
E(k
J/mol)
200
180
160
140
120
100
80
Ln(A(alpha)f(alpha)(1/s))(-)
45
40
35
30
25
20
15
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Temperature (C)
225220215210205200195190185180175170165160155150145140
Rea
ctionRate(-/s)
0.015
0.01
0.005
0
ReactionProg
ress(-)
1
0.8
0.6
0.4
0.2
0
0.125C/min 0.25C/min 0.5C/min 1C/min 2C/min 4C/min
0.125C/min 0.25C/min
0.5C/min
1C/min
2C/min
4C/min
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Simulation of the Reaction Progress (A) and ReactionSimulation of the Reaction Progress (A) and Reaction
Rate (B) Under NonRate (B) Under Non--Isothermal ConditionsIsothermal Conditions
(A)
(B)
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Simulation of the Reaction Progress (A) and ReactionSimulation of the Reaction Progress (A) and Reaction
Rate (B) Under Isothermal ConditionsRate (B) Under Isothermal Conditions
Time (h)
8.587.576.565.554.543.532.521.510.50
Rea
ctionRate(-/s)
3E-4
2E-4
1E-4
0
ReactionProg
ress(-)
1
0.8
0.6
0.4
0.2
0
175C
170C
165C
160C
175C 170C 165C 160C(A)
(B)
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TemperatureTemperature--Time Dependence forTime Dependence for
Different Sample MassesDifferent Sample Masses
with a fewwith a fewDSC or C80DSC or C80
experimentsexperiments
carried out oncarried out on
mgmg--scalescale
SADT
TMRad
Shelf-
life
mgmg
kgkg
tonton
To
=120C?
To
=120C?
Azodicarbonamide (CAS: 123-77-3)
To
=120C?
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19Proprietary property of Fauske & Associates, LLC
Heat Balance: Kilogram ScaleHeat Balance: Kilogram Scale
tC
H
r
T
r
g
r
T
rCt
T
p
r
p
1
Thermal
conductivity
?? Decompositionkinetics
Accumulation
reaction output accumulation
heat
conducted
in
heat
generated
within
heat
conducted
out
change in
energy
stored
within+ +=
Heat balance combined with numerical
analysis enables the determination ofthe
(i) heat accumulation and
(ii) reaction rate and progress
for any surrounding temperature profile
input
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Prediction of SADT Applying HeatPrediction of SADT Applying Heat
Balance & Kinetic DataBalance & Kinetic Data
Time (day)1086420
Temperature(C)
122
120
118
116
114
112
110
SADT=114C,50kg,1650kgm -3,1.05Jg^-1K^-1,0.1Wm -1K^-1,-1373.5Jg^-1,5Wm -2K^-1
overheat 6C
T surrounding -2 C
7 day or less
time = 6.49 day
SADT = 114 C
The SADT is 114C. This temperature is the lowest environment temperature at which overheat in the middle ofthe specific packaging exceeds 6C (T6) after a lapse of the period of seven days (168 hours) or less. This period
is measured from the time when the packaging center temperature reaches 2C below the surrounding
temperature. This overheat of 6C occurs after about 6.5 days.
centersurface
outside
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Simulation of Thermal Explosion of a 50 kgSimulation of Thermal Explosion of a 50 kg
Package of Azodicarbonamide (TPackage of Azodicarbonamide (Tambamb
= 120= 120C)C)
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SADT ResultsSADT Results
SADT predicted: 114C
SADT literature: 115C
(M.W. Whitmore, J.K. Wilberforce, J. Loss Prev. Process Ind., 6 (1993) 95)
The simulated SADT values of azodicarbonamide being in very good
agreement with those already determined indicate the
(i) correct collection of the experimental DSC data,
(ii) accurate procedure of the determination of kinetic parameters, and
(iii) precise evaluation of the thermal safety behavior implemented inAKTS-Thermokinetics software.
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