超聲波的縱波發射聲場
1.圓盤(pan)波(bo)(bo)源縱波(bo)(bo)聲(sheng)場 在不考(kao)慮介質中(zhong)衰(shuai)減(jian)的(de)情(qing)況下(xia),圓盤(pan)波(bo)(bo)源在理想液體介質中(zhong)振動輻射(she)聲(sheng)波(bo)(bo),其(qi)中(zhong)某一點(dian)(dian)波(bo)(bo)源d,在波(bo)(bo)源軸(zhou)(zhou)線上(shang)Q點(dian)(dian)所引起(qi)的(de)聲(sheng)壓(ya)為(wei)(圖2.13)基于(yu)波(bo)(bo)的(de)疊(die)加(jia)原(yuan)理,整個圓盤(pan)波(bo)(bo)源上(shang)各點(dian)(dian)在Q點(dian)(dian)引起(qi)的(de)聲(sheng)壓(ya)疊(die)加(jia),就是(shi)Q點(dian)(dian)處的(de)聲(sheng)壓(ya),由此可得到軸(zhou)(zhou)線上(shang)任一點(dian)(dian)的(de)聲(sheng)壓(ya)幅值為(wei)波(bo)(bo)源軸(zhou)(zhou)線...