超聲波的縱波發射聲場
1.圓盤(pan)(pan)波(bo)(bo)源(yuan)縱波(bo)(bo)聲場 在(zai)不考(kao)慮介質(zhi)(zhi)中(zhong)衰減的情況下,圓盤(pan)(pan)波(bo)(bo)源(yuan)在(zai)理(li)想液體介質(zhi)(zhi)中(zhong)振(zhen)動輻射(she)聲波(bo)(bo),其中(zhong)某(mou)一點(dian)(dian)(dian)波(bo)(bo)源(yuan)d,在(zai)波(bo)(bo)源(yuan)軸(zhou)(zhou)線(xian)(xian)上(shang)Q點(dian)(dian)(dian)所引(yin)起的聲壓為(圖2.13)基于波(bo)(bo)的疊加原理(li),整(zheng)個圓盤(pan)(pan)波(bo)(bo)源(yuan)上(shang)各(ge)點(dian)(dian)(dian)在(zai)Q點(dian)(dian)(dian)引(yin)起的聲壓疊加,就是Q點(dian)(dian)(dian)處的聲壓,由此可得(de)到軸(zhou)(zhou)線(xian)(xian)上(shang)任(ren)一點(dian)(dian)(dian)的聲壓幅值為波(bo)(bo)源(yuan)軸(zhou)(zhou)線(xian)(xian)...