Intimidate 发表于 2025-3-21 18:50:03
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Christoph Barchewitz,Thomas Armbrüstero u: = V. - V.. The velocity field shown in figure 2.1b is actually obtained from the velocity field shown in figure 2.1a by superimposing on it a velocity equal to the shock wave velocity but in the opposite direction. The flow field of figure 2.1b is pseudo-steady, and hence can be treated using tanchor 发表于 2025-3-22 20:49:54
Christoph Barchewitz,Thomas Armbrüster Detonation Shock Dynamics (JB Bdzil and DS Stewart) .The chapters are thematically interrelated in a systematic descriptive approach, though, each chapter is self-contained and can be read independently from the others. It offers a timely reference of theoretical detonation physics for graduate stMechanics 发表于 2025-3-22 21:44:02
Christoph Barchewitz,Thomas Armbrüster, .(.) is in . and . is a linear operator. The main example is the case where . is a linear elliptic operator. The “rest points” ., in this setting now are solutions of the equation . + .(.) = 0, and the linearized operator becomes . + . (.). We shall show that if the spectrum of this operator liesreception 发表于 2025-3-23 01:47:59
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pacts. Three novel approaches have been implemented: (1) shock consolidation of pre-heated specimens; (2) shock densification at a low pressure (just above threshold for pore collapse) followed by hot isostatic pressing (hipping); (3) use of local shock-induced reactions to increase temperatures of