Gutierrez M I, Lopez-Haro S A, Vera A, Leija L
CONACYT, Instituto Nacional de Rehabilitación, Subdirección de Investigación Tecnológica, Calz. México Xochimilco, No. 289, Col. Arenal de Guadalupe, Mexico City, Mexico.
Centro de Investigación y de Estudios Avanzados del IPN (Cinvestav-IPN), Electrical Engineering Department, Bioelectronics Section, Av. Instituto Politécnico Nacional 2508, Col. San Pedro Zacatenco, Del. Gustavo A. Madero, Mexico City, Mexico.
Biomed Res Int. 2016;2016:5484735. doi: 10.1155/2016/5484735. Epub 2016 Nov 23.
. To present a quantitative comparison of thermal patterns produced by the piston-in-a-baffle approach with those generated by a physiotherapy ultrasonic device and to show the dependency among thermal patterns and acoustic intensity distributions. . The finite element (FE) method was used to model an ideal acoustic field and the produced thermal pattern to be compared with the experimental acoustic and temperature distributions produced by a real ultrasonic applicator. A thermal model using the measured acoustic profile as input is also presented for comparison. Temperature measurements were carried out with thermocouples inserted in muscle phantom. The insertion place of thermocouples was monitored with ultrasound imaging. . Modeled and measured thermal profiles were compared within the first 10 cm of depth. The ideal acoustic field did not adequately represent the measured field having different temperature profiles (errors 10% to 20%). Experimental field was concentrated near the transducer producing a region with higher temperatures, while the modeled ideal temperature was linearly distributed along the depth. The error was reduced to 7% when introducing the measured acoustic field as the input variable in the FE temperature modeling. . Temperature distributions are strongly related to the acoustic field distributions.
. 对活塞在障板方法产生的热模式与物理治疗超声设备产生的热模式进行定量比较,并展示热模式与声强分布之间的相关性。. 采用有限元(FE)方法对理想声场和产生的热模式进行建模,以便与实际超声探头产生的实验声分布和温度分布进行比较。还提出了一个以测量的声剖面作为输入的热模型用于比较。使用插入肌肉模型中的热电偶进行温度测量。通过超声成像监测热电偶的插入位置。. 在深度的前10厘米内比较建模和测量的热剖面。理想声场不能充分代表具有不同温度剖面的测量场(误差为10%至20%)。实验场集中在换能器附近,产生一个温度较高的区域,而建模的理想温度沿深度呈线性分布。当在有限元温度建模中引入测量的声场作为输入变量时,误差降低到7%。. 温度分布与声场分布密切相关。