This paper demonstrates that the partial squeezing of car tire cavities at ground impact cannot he adequately modeled by the usual acoustic wave equation. A more complete treatment must begin with the Euler equations for fluid flow in a squeezed cavity to derive a wave equation dependent on cavity wall velocities and accelerations. These can be sizable as ground impact causes the walls of a tire cavity to move with velocities of order 1 m/s and with accelerations of 10(3) m/s(2) over time scales of about 1 ms. Further, the geometry of a typical cavity is such that width compression causes significant increases in pressure and density to occur before the arrival of the rarefaction wave propagating from the open end of the cavity begins to exhaust the full length of the cavity. This causes significant departures from equilibrium density and pressure conditions. These influences are demonstrated both analytically and numerically. (C) 1999 Acoustical Society of America. [S0001-4966(99)00708-0].
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机译:本文证明了在地面撞击时汽车轮胎腔的局部挤压不能通过通常的声波方程充分建模。必须从欧拉方程开始更完整的处理,以使流体在挤压腔中流动,从而得出取决于腔壁速度和加速度的波动方程。当地面撞击导致轮胎腔壁以1 m / s的速度移动并且在大约1 ms的时间范围内以10(3)m / s(2)的加速度移动时,这些影响可能很大。此外,典型腔的几何形状使得宽度压缩导致从腔的开口端传播的稀疏波的到达开始耗尽腔的整个长度之前,压力和密度显着增加。这导致明显偏离平衡密度和压力条件。这些影响在分析和数值上都得到了证明。 (C)1999年美国声学学会。 [S0001-4966(99)00708-0]。
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