超聲波的縱波發射聲場
1.圓盤(pan)(pan)波(bo)(bo)(bo)源(yuan)縱波(bo)(bo)(bo)聲場(chang) 在不考慮介質中衰減(jian)的(de)情況下,圓盤(pan)(pan)波(bo)(bo)(bo)源(yuan)在理想(xiang)液(ye)體介質中振(zhen)動輻射聲波(bo)(bo)(bo),其(qi)中某一點(dian)(dian)波(bo)(bo)(bo)源(yuan)d,在波(bo)(bo)(bo)源(yuan)軸(zhou)線上Q點(dian)(dian)所引起(qi)的(de)聲壓為(圖2.13)基于波(bo)(bo)(bo)的(de)疊(die)加原理,整個圓盤(pan)(pan)波(bo)(bo)(bo)源(yuan)上各點(dian)(dian)在Q點(dian)(dian)引起(qi)的(de)聲壓疊(die)加,就(jiu)是Q點(dian)(dian)處的(de)聲壓,由此可得到軸(zhou)線上任一點(dian)(dian)的(de)聲壓幅(fu)值(zhi)為波(bo)(bo)(bo)源(yuan)軸(zhou)線...