Oelze Michael L, Miller Rita J, Blue James P, Zachary James F, O'Brien William D
Bioacoustics Research Laboratory, Department of Electrical and Computer Engineering, University of Illinois, 405 North Mathews, Urbana, Illinois 61801, USA.
J Acoust Soc Am. 2008 Oct;124(4):2340-52. doi: 10.1121/1.2973186.
In a previous study, it was hypothesized that ultrasound-induced lung damage was related to the transfer of ultrasonic energy into the lungs (W. D. O'Brien et al. 2002, "Ultrasound-induced lung hemorrhage: Role of acoustic boundary conditions at the pleural surface," J. Acoust. Soc. Am. 111, 1102-1109). From this study a technique was developed to: 1) estimate the impedance (Mrayl) of fresh, excised, ex vivo rat lung versus its level of inflation (cm H(2)O) and 2) predict the fraction of ultrasonic energy transmitted into the lung (M. Oelze et al. 2003, "Impedance measurements of ex vivo rat lung at different volumes of inflation." J. Acoust. Soc. Am. 114, 3384-3393). In the current study, the same technique was used to estimate the frequency-dependent impedance of lungs from rats, rabbits, and pigs of various ages. Impedance values were estimated from lungs under deflation (atmospheric pressure, 0 cm H(2)O) and three volumes of inflation pressure [7 cm H(2)O (5 cm H(2)O for pigs), 10 cm H(2)O, and 15 cm H(2)O]. Lungs were scanned in a tank of degassed 37 degrees C water. The frequency-dependent acoustic pressure reflection coefficient was determined over a frequency range of 3.5-10 MHz. From the reflection coefficient, the frequency-dependent lung impedance was calculated with values ranging from an average of 1.4 Mrayl in deflated lungs (atmospheric pressure) to 0.1 Mrayl for fully inflated lungs (15 cm H(2)O). Across all species, deflated lung (i.e., approximately 7% of the total lung capacity) had impedance values closer to tissue values, suggesting that more acoustic energy was transmitted into the lung under deflated conditions. Finally, the impedance values of deflated lungs from different species at different ages were compared with the thresholds for ultrasound-induced lung damage. The comparison revealed that increases in ultrasonic energy transmission corresponded to lower injury threshold values.
在之前的一项研究中,曾有假设认为超声引起的肺损伤与超声能量向肺内的传递有关(W.D.奥布赖恩等人,2002年,《超声引起的肺出血:胸膜表面声学边界条件的作用》,《美国声学学会杂志》第111卷,第1102 - 1109页)。基于该研究开发了一种技术,用于:1)估计新鲜的、离体的大鼠肺相对于其充气水平(厘米水柱)的声阻抗(瑞利),以及2)预测传入肺内的超声能量分数(M.厄尔泽等人,2003年,《不同充气量下离体大鼠肺的阻抗测量》,《美国声学学会杂志》第114卷,第3384 - 3393页)。在当前研究中,使用相同技术估计不同年龄大鼠、兔子和猪肺的频率依赖性阻抗。在肺处于放气状态(大气压,0厘米水柱)以及三个充气压力值[7厘米水柱(猪为5厘米水柱)、10厘米水柱和15厘米水柱]下估计阻抗值。在装有37℃脱气水的水槽中对肺进行扫描。在3.5 - 10兆赫的频率范围内测定频率依赖性声压反射系数。根据反射系数计算频率依赖性肺阻抗,其值范围从放气肺(大气压)的平均1.4瑞利到完全充气肺(15厘米水柱)的0.1瑞利。在所有物种中,放气肺(即约占肺总容量的7%)的阻抗值更接近组织值,这表明在放气条件下有更多声能传入肺内。最后,将不同物种不同年龄放气肺的阻抗值与超声引起肺损伤的阈值进行比较。比较结果显示,超声能量传递的增加对应着更低的损伤阈值。