超聲波的縱波發射聲場
1.圓(yuan)盤(pan)波(bo)(bo)源(yuan)(yuan)縱波(bo)(bo)聲(sheng)(sheng)(sheng)場(chang) 在(zai)不考慮(lv)介質中衰(shuai)減的情況下,圓(yuan)盤(pan)波(bo)(bo)源(yuan)(yuan)在(zai)理想液(ye)體介質中振動輻射聲(sheng)(sheng)(sheng)波(bo)(bo),其中某一點(dian)波(bo)(bo)源(yuan)(yuan)d,在(zai)波(bo)(bo)源(yuan)(yuan)軸(zhou)線(xian)上Q點(dian)所引起(qi)的聲(sheng)(sheng)(sheng)壓(ya)為(wei)(圖2.13)基于波(bo)(bo)的疊加原理,整個圓(yuan)盤(pan)波(bo)(bo)源(yuan)(yuan)上各點(dian)在(zai)Q點(dian)引起(qi)的聲(sheng)(sheng)(sheng)壓(ya)疊加,就是(shi)Q點(dian)處的聲(sheng)(sheng)(sheng)壓(ya),由此可(ke)得(de)到(dao)軸(zhou)線(xian)上任一點(dian)的聲(sheng)(sheng)(sheng)壓(ya)幅值為(wei)波(bo)(bo)源(yuan)(yuan)軸(zhou)線(xian)...