超聲波的縱波發射聲場
1.圓盤(pan)(pan)波(bo)(bo)(bo)(bo)源(yuan)(yuan)(yuan)縱(zong)波(bo)(bo)(bo)(bo)聲(sheng)(sheng)場 在不(bu)考慮介質中(zhong)衰(shuai)減的(de)(de)情況下,圓盤(pan)(pan)波(bo)(bo)(bo)(bo)源(yuan)(yuan)(yuan)在理想液體介質中(zhong)振動(dong)輻射聲(sheng)(sheng)波(bo)(bo)(bo)(bo),其中(zhong)某一(yi)點(dian)(dian)波(bo)(bo)(bo)(bo)源(yuan)(yuan)(yuan)d,在波(bo)(bo)(bo)(bo)源(yuan)(yuan)(yuan)軸(zhou)線上Q點(dian)(dian)所引起的(de)(de)聲(sheng)(sheng)壓為(圖2.13)基于(yu)波(bo)(bo)(bo)(bo)的(de)(de)疊加(jia)原(yuan)理,整個圓盤(pan)(pan)波(bo)(bo)(bo)(bo)源(yuan)(yuan)(yuan)上各點(dian)(dian)在Q點(dian)(dian)引起的(de)(de)聲(sheng)(sheng)壓疊加(jia),就(jiu)是Q點(dian)(dian)處的(de)(de)聲(sheng)(sheng)壓,由此可得(de)到軸(zhou)線上任(ren)一(yi)點(dian)(dian)的(de)(de)聲(sheng)(sheng)壓幅(fu)值為波(bo)(bo)(bo)(bo)源(yuan)(yuan)(yuan)軸(zhou)線...