2008
DOI: 10.1134/s1063771008010065
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Nonlinear spherically divergent shock waves propagating in a relaxing medium

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Cited by 19 publications
(45 citation statements)
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“…17,18 Nevertheless, the N-wave model is widespread to describe pressure signatures of shock pulses during their propagation in air. 11,12,19 Even if the waveform is not restricted to have the N-wave shape in simulations of pulse propagation through homogeneous 12 and turbulent media, 20 the N-wave assumption is still often used to set a boundary condition to the model. This simplified assumption may introduce errors, for example, in the simulation of pulse propagation through a caustic, in which the resulting waveform resembles the derivative of an initial wave.…”
Section: Introductionmentioning
confidence: 99%
“…17,18 Nevertheless, the N-wave model is widespread to describe pressure signatures of shock pulses during their propagation in air. 11,12,19 Even if the waveform is not restricted to have the N-wave shape in simulations of pulse propagation through homogeneous 12 and turbulent media, 20 the N-wave assumption is still often used to set a boundary condition to the model. This simplified assumption may introduce errors, for example, in the simulation of pulse propagation through a caustic, in which the resulting waveform resembles the derivative of an initial wave.…”
Section: Introductionmentioning
confidence: 99%
“…2(b) where ϵ = 1 × 10 −5 and there was good agreement between the asymptotic predictions and numerical results. Laboratory measurements for a spherically spreading shock generated by an electrical spark source [27] correspond to ϵ ≈ 1 × 10…”
Section: Discussionmentioning
confidence: 99%
“…Thus we have two separate predictions from the asymptotic analysis to be compared with the full numerical solutions. For smaller times we have the Taylor shock width (26), whereas for larger times we have the shock width obtained from the error function shock form (27).…”
Section: Spherical Casementioning
confidence: 99%
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“…Its front shock rise time which is unaffected by the turbulence interaction are less than approximately 3 μs, and it corresponds with a wave duration on the order of less than 1/10; thus, the short shock rise time is in high frequency domain. Wave attenuation, which is important factor for a shock wave propagation, depends on the frequency component which the pressure waveform has [31]. The frequency component of the short rise time does not correspond with that of the long rise time enable us to deduce that the same shock wave focusing/diffracting effects do not necessarily contribute to the long risetime pressure signature.…”
Section: Introductionmentioning
confidence: 99%