超聲波的縱波發射聲場
1.圓(yuan)盤(pan)波源(yuan)(yuan)縱波聲(sheng)場 在不考慮介(jie)質(zhi)中衰減(jian)的情況下,圓(yuan)盤(pan)波源(yuan)(yuan)在理想液體介(jie)質(zhi)中振(zhen)動輻射聲(sheng)波,其(qi)中某一點(dian)(dian)波源(yuan)(yuan)d,在波源(yuan)(yuan)軸(zhou)(zhou)(zhou)線(xian)(xian)上Q點(dian)(dian)所引(yin)起的聲(sheng)壓(ya)為(圖2.13)基(ji)于波的疊加原理,整(zheng)個(ge)圓(yuan)盤(pan)波源(yuan)(yuan)上各(ge)點(dian)(dian)在Q點(dian)(dian)引(yin)起的聲(sheng)壓(ya)疊加,就是(shi)Q點(dian)(dian)處的聲(sheng)壓(ya),由此可得到(dao)軸(zhou)(zhou)(zhou)線(xian)(xian)上任(ren)一點(dian)(dian)的聲(sheng)壓(ya)幅(fu)值為波源(yuan)(yuan)軸(zhou)(zhou)(zhou)線(xian)(xian)...