Tailoring of High Energy Materials: Part 02: GPeng Model
Gayatri Patel
Final
Year B Tech Student
ITER,
Bhubaneswar, INDIA
and
Dr Manoj K Patel
Asst
Vice President, Reliance Sasan Power Limited, Sasan, INDIA
Mobile
No: +91 8249206647
Email
ID: manjubeti@rediffmail.com
INTRODUCTION:
“Chemicals” and “mixture of chemicals” that
are high energetic materials need special attention. This category subsumes –
pyrotechnics and explosives (initiating devices included). These categories of
materials have their unique thermodynamic properties.
Thermodynamic properties of high energetic
materials can be measured both experimentally as well as through theoretical
means. Both the methods have got their own advantages and dis-advantages.
Experimental methods are based on very
sophisticated equipments and now a days these are available on PLC Control
basis. Results can be obtained within a time frame of 30 minutes per sample.
But these experimental methods need high end laboratory, expensive equipments
and skilled instrumentation engineer to conduct the experiments. Moreover, the
experimental method needs high energy materials to be handled in a chemical
laboratory time and again. Additionally, state statutes and
safety-security-issues come in to picture in terms of licenses to handle high
energetic materials in the laboratory. Hence attempts have been made in the
past for effective, theoretical calculations of the detonation parameters and
the chemical equilibrium composition of reaction products.
Alternate way thus is to go for – Theoretical
Methods. Survey of literature showed that a number of theoretical methods have
been available for carrying out thermodynamic calculations of the detonation
parameters of condensed explosives. Some of these are, a BKW Fortran [1],
ARPEGE [2], Ruby [3], TIGER [4], CHEETAH [5], EXPLO5 [6], MWEQ [7], BARUT-X
[8]. Although in many research centers in the world thermo-chemical codes were
worked out, access to them is difficult and, moreover, any changes in the codes
aren’t possible because they are made available in the compiled form.
Therefore, we have worked out and have come up with our own numerical code
named GPeng from
which one can derive as many as 18 different parameters for a “chemical” or
“mixture of chemicals”.
THE GPeng MODEL:
Our GPeng is a new model for calculation of thermodynamic properties of chemicals,
mixture of chemicals, high energetic materials and pyrotechnics. GPeng is based on such facts as: (a) physical and chemical properties of an
energetic material, (b) its atomic composition, (c) enthalpy of formation, (d)
entropy of chemicals, (e) molecular reaction dynamics, (f) the mathematical
model of an ideal detonation, (g) the principle of extreme of characteristic
functions delineated by Gibbs, and (h) thermodynamic equations of state for the
real gasses (reaction products) with a wide range of pressure and temperature.
In its present form GPeng is
able to determine 18 different thermodynamic parameters and these are:
No
|
Output Parameter from “GPeng”
|
UoM
|
01
|
OF (Oxygen Balance Factor)
|
No.
|
02
|
SF (Strength Factor)
|
No.
|
03
|
del H (Enthalpy)
|
Kcal/kg
|
04
|
So (Entropy)
|
Cal
|
05
|
Gibbs Free Energy
|
Kcal/kg
|
06
|
Volume Expansion Considering Water is Gas
|
Percent
|
07
|
Volume Expansion Considering Water is
Liquid
|
Percent
|
08
|
Mole of Oxygen Generated from Decomposition
of OB
|
Mole/kg of Product
|
09
|
Mole of Oxygen Required for Complete
Combustion of FB
|
Mole/kg of Product
|
10
|
Mole of Gases Generated from OB
|
Mole/kg of Product
|
11
|
Mole of Gases Generated from FB
|
Mole/kg of Product
|
12
|
Mole of Gases Generated from Composition
|
Mole/kg of Product
|
13
|
Absolute Bulk Strength or
ABS
|
Kcal/cubic meter
|
14
|
Absolute Weight Strength (i.e. del H)
|
Kcal/kg
|
15
|
Relative Bulk Strength wrt ANFO or
RBS_ANFO
|
Percent
|
16
|
Relative Weight Strength wrt ANFO or RWS_ANFO
|
Percent
|
17
|
Relative Bulk Strength wrt NG or
RBS_NG
|
Percent
|
18
|
Relative Weight Strength wrt NG or
RWS_NG
|
Percent
|
To verify the GPeng Model, its results are compared with that obtained from the experimental
methods by using a Parr 6100 Calorimeter.
We are further going to develop this model– (1)
to calculate the parameters of combustion, explosion and detonation of
condensed energetic materials, (2) to determine the curve of expansion of detonation
products, (3) to arrive at a correlation between the parameters obtained
through GPeng
with Rock Characteristics (GPengRock).
APPLICATION OF GPeng in SOME CHEMICALS:
(1) Ammonium Nitrate (AN):
Ammonium
Nitrate is having chemical formula NH4NO3 and its structure is:
On
explosion, it undergoes the reaction of:
Species Name
|
Image
|
ΔfH°(0 K)
|
ΔfH°(298.15 K)
|
Units
|
Relative
Molecular Mass |
|
(NH4)NO3
|
-350.28
|
-365.25
|
kcal/kg
|
80.04344 ±
0.00095 |
This reaction path has been considered in the
GPeng and
the values obtained are:
Results for AN
|
||
Output Parameter
|
UoM
|
RESULT
|
SF
|
No.
|
0
|
del H (i.e. Enthalpy)
|
Kcal/kg
|
-353
|
So (i.e. Entropy)
|
Cal
|
1555
|
Gibbs Free Energy
|
Kcal/kg
|
-399
|
Volume Expansion
Considering Water is Gas
|
Percent
|
350
|
Volume Expansion
Considering Water is Liquid
|
Percent
|
150
|
Mole of Oxygen Generated
from Decomposition of OB
|
Mole/kg of Product
|
15.63
|
Mole of Oxygen Required
for Complete Combustion of FB
|
Mole/kg of Product
|
0
|
Mole of Gases Generated
from OB
|
Mole/kg of Product
|
162.45
|
Mole of Gases Generated
from FB
|
Mole/kg of Product
|
0
|
Mole of Gases Generated
from Composition
|
Mole/kg of Product
|
162.45
|
Absolute Bulk
Strength or ABS
|
Kcal/cubic meter
|
-395
|
Absolute Weight
Strength (i.e. del H)
|
Kcal/kg
|
-353
|
Relative Bulk
Strength wrt ANFO or RBS_ANFO
|
Percent
|
51
|
Relative Weight Strength
wrt ANFO or RWS_ANFO
|
Percent
|
34
|
Relative Bulk
Strength wrt NG or RBS_NG
|
Percent
|
19
|
Relative Weight
Strength wrt NG or RWS_NG
|
Percent
|
24
|
(2) Ammonium Nitrate Fuel Oil (ANFO):
ANFO in its best form is - 94.5% of AN and 5.5% of Diesel
Oil. When this mixture undergoes explosion, it releases lot of energy, and its
output thermodynamics parameters also have been calculated by using GPeng.
Findings are as follows:
RESULTS for ANFO
|
||
Output Parameter
|
UoM
|
RESULT
|
SF
|
No.
|
18.81
|
del H (i.e. Enthalpy)
|
Kcal/kg
|
-917
|
So (i.e. Entropy)
|
Cal
|
1517
|
Gibbs Free Energy
|
Kcal/kg
|
-963
|
Volume Expansion
Considering Water is Gas
|
Percent
|
374.75
|
Volume Expansion
Considering Water is Liquid
|
Percent
|
97.75
|
Mole of Oxygen Generated
from Decomposition of OB
|
Mole/kg of Product
|
14.77
|
Mole of Oxygen Required
for Complete Combustion of FB
|
Mole/kg of Product
|
39.53
|
Mole of Gases Generated
from OB
|
Mole/kg of Product
|
153.52
|
Mole of Gases Generated
from FB
|
Mole/kg of Product
|
67.64
|
Mole of Gases Generated
from Composition
|
Mole/kg of Product
|
221.15
|
Absolute Bulk
Strength or ABS
|
Kcal/cubic meter
|
-1027
|
Absolute Weight
Strength (i.e. del H)
|
Kcal/kg
|
-917
|
Relative Bulk
Strength wrt ANFO or RBS_ANFO
|
Percent
|
132
|
Relative Weight Strength
wrt ANFO or RWS_ANFO
|
Percent
|
89
|
Relative Bulk
Strength wrt NG or RBS_NG
|
Percent
|
49
|
Relative Weight
Strength wrt NG or RWS_NG
|
Percent
|
62
|
(2) An Emulsion Explosives Formulation:
One of the Site Mixed Emulsions (SME) has been designed with
chemical parameters in the percentage level of: AN 72 / SN 05 / Water 15.5 /
HSD 03 / FO 03 / Emulsifier 01.2 / Wax 0.2.
This mixture was prepared in the laboratory and its
enthalpy was measured experimentally with the help of Parr 6100 fully automatic
bomb calorimeter.
Bomb calorimeter showed enthalpy of 832 Kcal/kg and GPeng
showed that at 840 Kcal/kg. Values thus obtained experimentally and
theoretically are very close to each other and rather with 95% confidence
limit.
The other values determined for this formulation using GPeng, the
output results are as follows:
RESULTS for the above SME
Formulation
|
||
Output Parameter
|
UoM
|
RESULT
|
SF
|
No.
|
16.76
|
del H (i.e. Enthalpy)
|
Kcal/kg
|
-840
|
So (i.e. Entropy)
|
Cal
|
1518
|
Gibbs Free Energy
|
Kcal/kg
|
-885
|
Volume Expansion
Considering Water is Gas
|
Percent
|
347.36
|
Volume Expansion
Considering Water is Liquid
|
Percent
|
70.34
|
Mole of Oxygen Generated
from Decomposition of OB
|
Mole/kg of Product
|
15.16
|
Mole of Oxygen Required
for Complete Combustion of FB
|
Mole/kg of Product
|
52.78
|
Mole of Gases Generated
from OB
|
Mole/kg of Product
|
131.27
|
Mole of Gases Generated
from FB
|
Mole/kg of Product
|
91.13
|
Mole of Gases Generated
from Composition
|
Mole/kg of Product
|
222.40
|
Absolute Bulk
Strength or ABS
|
Kcal/cubic meter
|
-940
|
Absolute Weight
Strength (i.e. del H)
|
Kcal/kg
|
-840
|
Relative Bulk
Strength wrt ANFO or RBS_ANFO
|
Percent
|
121
|
Relative Weight Strength
wrt ANFO or RWS_ANFO
|
Percent
|
82
|
Relative Bulk
Strength wrt NG or RBS_NG
|
Percent
|
45
|
Relative Weight
Strength wrt NG or RWS_NG
|
Percent
|
56
|
Values thus obtained in the above three cases are
compared with the experimental values obtained in Bomb Calorimeter. GPeng
values are matching with Bomb Calorimeter values to the level of 95% confidence
limit.
So, one NEED NOT SPEND lot of time and cost for
determining the parameters by using expensive lab equipments. GPeng
itself gives rise to these values with good accuracies. The authors, however,
welcome suggestions and comments from researchers and explosives scientists in
order to fine tune the GPeng further.
REFERENCES:
[1] Mader Ch.J., FORTRAN BKW: a code computing
the detonation properties of explosives, Los Alamos Science Laboratory, Report
LA-3704, 1967.
[2] Cheret R., The numerical study of the
detonation products of an explosive substance, French Commission of Atomic
Energy, Report CEA-R-4122, 1971.
[3] Levin H.B., Sharples R.E., Operator’s
manual for RUBY, Lawrence Livermore Laboratory, Report UCRL-6815, 1962.
[4] Cowperthwaite M., Zwisler W.H., Tiger
computer program documentation, Stanford Research Institute, Publication
No. Z106, 1973.
[5] Fried L.E., CHEETAH 1.39 User’s Manual,
Lawrence Livermore National Laboratory, Manuscript UCRL-MA-117541 Rev. 3, 1996.
[6] Sućeska M., Calculation of the detonation
properties of C-H-N-O explosives, Propellants Explos. Pyrotech., 1991,
16, 197-202.
[7] Papliński A., Equilibrium thermochemical
calculations for a great mount of components (in Polish), Biul. WAT, 1993,
42(11), 123-143.
[8] Cengiz F., Narin B., Ulas A., BARUT-X: a
computer code for computing the steady-state detonation properties of condensed
phase explosives, 10th Seminar New Trends in Energetic Materials,
Pardubice, 2007, 117-127.
[9]
|
S. J. Klippenstein, L. B.
Harding, and B. Ruscic, Ab initio Computations and Active Thermochemical
Tables Hand in Hand: Heats of Formation of Core Combustion Species. J.
Phys. Chem. A in preparation (2016).
|
|
[10]
|
B.
Ruscic, Uncertainty Quantification in Thermochemistry, Benchmarking
Electronic Structure Computations, and Active Thermochemical Tables. Int.
J. Quantum Chem. 114, 1097-1101 (2014).
|
|
[11]
|
Ab Initio Computations and
Active Thermochemical Tables Hand in Hand: Heats of Formation of Core Combustion Species, Stephen J. Klippenstein, Lawrence B.
Harding, and Branko Ruscic, Chemical
Sciences and Engineering Division, Argonne National Laboratory, Argonne,
Illinois 60439, United States, J. Phys. Chem.
A, 2017, 121 (35), pp 6580–6602,
DOI: 10.1021/acs.jpca.7b05945, Publication Date (Web): July 31, 2017.
|
[12]
Zygmunt B., Buczkowski D., Influence of Ammonium Nitrate Prills Properties on Detonation
Velocity of ANFO, Propellants, Explos., Pyrotech., 2007, 32(5), 411-414.
[13] Buczkowski D., Zygmunt B., Influence of
Ammonium Nitrate Prills’ Porosity and Dimesions on Detonation Velocity of ANFO
Explosives, Vth Int. Seminar “New Trends in Research of Energetic Materials”,
Pardubice, 21-23.04.2003, 45-51.
[14] Trzciński
W.A., Cudziło S., The Application of the Cylinder Test to Determine the Energy
Characteristics of Industrial Explosives, Archives of Mining Sciences, (2001),
46(3), 291-307.
[15] Buczkowski
D., Trzciński W. A., Zygmunt B., Examining of Energetic Properties of ANFO
Explosive by Using Cylindrical Test, Fifth Int. Armament Conf. Scientific
Aspects of Armament”, Waplewo, 9-11.10.2004, 74-82.
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