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Fig. 9.18 Plots of the
decomposition rate of the
AP-PS mixture (second
stage) against the temperature
at P = 10 5 Pa ( 1 ), 1 MPa ( 2 )
2
4.0
3.5
3.0
2.5
2.0 1.35
1.45
k 2 = 10 9 . 8 ± 0 . 5 exp
s 1 .
40900
±
1500
(9.6)
R T
The same pattern was observed for the NG-2-60-DTM material (Fig. 9.19). The
influence of the ambient pressure on the first-stage process was found to be similar
but much weaker.
Fig. 9.19 Effect of P
on the
min -1
rate of NG-2-60-DTM
decomposition: 1 and 2 ,
P = 10 5 Pa; 3 and 4 ,
P = 1MPa; 1 and 3 ,
ω
0.20
0.15
= 2 . 9 deg min 1 ; 2 and 4 ,
= 3 . 4 deg min 1
ω
0.1
0.05
9.4 Mechanism of High-Temperature Decomposition
of AP-Based Model Mixtures and Composite Solid
Propellants
The data on the thermal decomposition of the heterogeneous condensed systems
studied indicate a complex process. The decomposition of AP and most of the mix-
tures occurs via two stages, with the exception of the AP (coarse)-PE system, which
decomposes in a single stage. The organic binder mainly influences the first stage of
AP decomposition. For the AP-PS, AP-PAN and AP-PVC mixtures, the first de-
composition stage ( Q 1 = 0 . 2-0 . 5kJg 1 , E 1 = 133-142 kJ mol 1 , T 1 = 290-370 C)
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