1976
DOI: 10.1007/bf00743174
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Model of the nucleus of a multifront gas detonation

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Cited by 17 publications
(13 citation statements)
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“…In the limit case of cellular detonation propagation in gas mixtures, the decay of the detonation front on the segment between the converging transverse waves reaches the detonation-failure point, and a collision of transverse waves leads to reinitiation in the form of a strongly overdriven detonation wave. (A corresponding model of the detonation cell and a method for estimating the cell size, based on conditions of ignition failure, were proposed in [17].) The above-given results for gas suspensions of aluminum particles show that such a regime is not formed in bidisperse gas suspensions.…”
Section: Estimation Of the Size Of Cellular-type Structures By Means mentioning
confidence: 93%
“…In the limit case of cellular detonation propagation in gas mixtures, the decay of the detonation front on the segment between the converging transverse waves reaches the detonation-failure point, and a collision of transverse waves leads to reinitiation in the form of a strongly overdriven detonation wave. (A corresponding model of the detonation cell and a method for estimating the cell size, based on conditions of ignition failure, were proposed in [17].) The above-given results for gas suspensions of aluminum particles show that such a regime is not formed in bidisperse gas suspensions.…”
Section: Estimation Of the Size Of Cellular-type Structures By Means mentioning
confidence: 93%
“…For most practically important cases where inequalities (4) are valid, it is possible to show that the proportionality coefficients ahead of the derivative dD dt are negative. In conclusion, we note that except for the practical importance noted in [7,8], the gradient relations obtained in this work can be used in engineering calculations to estimate the values of the derivatives ∂y ∂r * from changes in the velocity of shock or detonation fronts recorded in experiments. In addition, they can be used to construct difference schemes of numerical algorithms near a moving boundary of the type of a shock (detonation) front.…”
Section: Prokhorovmentioning
confidence: 94%
“…For one-dimensional adiabatic flow of a perfect gas, such gradient relations at the shockwave front are given in [5,6]. These relations can be used to develop numerical and analytical approximate methods for solving gas-dynamic problems and establishing asymptotic laws of attenuation of shock waves [7,8]. Here it is also pertinent to note a paper on a related topic [9], in which spatial derivatives were obtained for gas-dynamic functions behind a curved stationary shock wave subjected to an oncoming uniform supersonic flow.…”
mentioning
confidence: 99%
“…The losses due to friction and heat transfer to the tube walls are ignored. The latter is caused by the fact that the Vasil'ev-Nikolaev model for calculating the detonationcell size [8,[37][38][39], which is used below, involves the wave parameters without losses on the walls.…”
Section: Detonation-wave Parameters and Cell Size In Gas Mixtures Witmentioning
confidence: 99%
“…According to the model developed in [8,[37][38][39], the longitudinal size of the gas-detonation cell b p depends on the wave velocity and gas parameters (pressure and temperature) behind the leading shock front as…”
Section: Detonation-wave Parameters and Cell Size In Gas Mixtures Witmentioning
confidence: 99%