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Products, detonation measured” product compositions

PETN density favors Mader s detonation product computations since, as shown above, Mader calculates that the amount of free carbon decreases with a decrease in PETN packing density The product compns measured by Ornellas (Table 8) and the Mader CJ compositions differ appreciably. The Q s are, however, very similar. The agreement between calorimeter and computed Q s is certainly unexpected in view of the different product compns. Nevertheless, as stated in Vol 7, H38—39, there is rather good agreement between calorimeter Q s for confined samples and the CJ Q s computed by Mader (Ref 40) for expls that are not too deficient in oxygen. The following tabulation illustrates this ... [Pg.577]

The measuring system used for the determination of detonation product composition is shown in Figure 4.75. [Pg.163]

Preceding discussions (in this chapter and Chapter 8) relate to problems attending the measurement of propagation rates in heavy-metal azides. The alternative of calculating the maximum, steady-state detonation rates in these azides from first principles is not well established. Nevertheless, a one-dimensional thermohydrodynamic model does exist which can yield reasonable values for detonation properties (velocity, pressure, product density and composition, particle velocity, etc.) [113-119]. [Pg.484]


See other pages where Products, detonation measured” product compositions is mentioned: [Pg.369]    [Pg.286]    [Pg.18]    [Pg.19]    [Pg.26]    [Pg.258]    [Pg.30]    [Pg.244]    [Pg.578]    [Pg.18]    [Pg.19]    [Pg.26]    [Pg.369]    [Pg.378]    [Pg.454]    [Pg.690]    [Pg.390]    [Pg.488]    [Pg.83]    [Pg.25]    [Pg.135]   


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