超聲波的縱波發射聲場
1.圓(yuan)(yuan)盤(pan)波(bo)源(yuan)縱(zong)波(bo)聲(sheng)(sheng)場 在不(bu)考慮介質中(zhong)(zhong)衰減的(de)(de)情況下,圓(yuan)(yuan)盤(pan)波(bo)源(yuan)在理(li)想液體介質中(zhong)(zhong)振動輻(fu)射聲(sheng)(sheng)波(bo),其(qi)中(zhong)(zhong)某一(yi)點(dian)波(bo)源(yuan)d,在波(bo)源(yuan)軸(zhou)線上(shang)Q點(dian)所引(yin)起(qi)的(de)(de)聲(sheng)(sheng)壓為(wei)(圖2.13)基于波(bo)的(de)(de)疊(die)加(jia)原理(li),整(zheng)個(ge)圓(yuan)(yuan)盤(pan)波(bo)源(yuan)上(shang)各(ge)點(dian)在Q點(dian)引(yin)起(qi)的(de)(de)聲(sheng)(sheng)壓疊(die)加(jia),就是Q點(dian)處的(de)(de)聲(sheng)(sheng)壓,由此可得到(dao)軸(zhou)線上(shang)任一(yi)點(dian)的(de)(de)聲(sheng)(sheng)壓幅值為(wei)波(bo)源(yuan)軸(zhou)線...