超聲波的縱波發射聲場
1.圓盤(pan)波(bo)源(yuan)縱波(bo)聲場 在(zai)(zai)(zai)不考(kao)慮介(jie)質(zhi)中(zhong)衰減(jian)的(de)(de)情況下,圓盤(pan)波(bo)源(yuan)在(zai)(zai)(zai)理想液體(ti)介(jie)質(zhi)中(zhong)振(zhen)動輻射聲波(bo),其中(zhong)某一(yi)點(dian)(dian)(dian)波(bo)源(yuan)d,在(zai)(zai)(zai)波(bo)源(yuan)軸(zhou)線(xian)上Q點(dian)(dian)(dian)所(suo)引起(qi)(qi)的(de)(de)聲壓(ya)為(wei)(圖2.13)基于波(bo)的(de)(de)疊加原理,整個圓盤(pan)波(bo)源(yuan)上各點(dian)(dian)(dian)在(zai)(zai)(zai)Q點(dian)(dian)(dian)引起(qi)(qi)的(de)(de)聲壓(ya)疊加,就是Q點(dian)(dian)(dian)處的(de)(de)聲壓(ya),由此可得到軸(zhou)線(xian)上任一(yi)點(dian)(dian)(dian)的(de)(de)聲壓(ya)幅值為(wei)波(bo)源(yuan)軸(zhou)線(xian)...