Deshazer Garron, Prakash Punit, Merck Derek, Haemmerich Dieter
a Department of Diagnostic Imaging , Rhode Island Hospital , Providence , Rhode Island , USA.
b Department of Electrical and Computer Engineering , Kansas State University , Manhattan , Kansas , USA.
Int J Hyperthermia. 2017 Feb;33(1):74-82. doi: 10.1080/02656736.2016.1206630. Epub 2016 Jul 18.
For computational models of microwave ablation (MWA), knowledge of the antenna design is necessary, but the proprietary design of clinical applicators is often unknown. We characterised the specific absorption rate (SAR) during MWA experimentally and compared to a multi-physics simulation.
An infrared (IR) camera was used to measure SAR during MWA within a split ex vivo liver model. Perseon Medical's short-tip (ST) or long-tip (LT) MWA antenna were placed on top of a tissue sample (n = 6), and microwave power (15 W) was applied for 6 min, while intermittently interrupting power. Tissue surface temperature was recorded via IR camera (3.3 fps, 320 × 240 resolution). SAR was calculated intermittently based on temperature slope before and after power interruption. Temperature and SAR data were compared to simulation results.
Experimentally measured SAR changed considerably once tissue temperatures exceeded 100 °C, contrary to simulation results. The ablation zone diameters were 1.28 cm and 1.30 ± 0.03 cm (transverse), and 2.10 cm and 2.66 ± -0.22 cm (axial), for simulation and experiment, respectively. The average difference in temperature between the simulation and experiment were 5.6 °C (ST) and 6.2 °C (LT). Dice coefficients for 1000 W/kg SAR iso-contour were 0.74 ± 0.01 (ST) and 0.77 (± 0.03) (LT), suggesting good agreement of SAR contours.
We experimentally demonstrated changes in SAR during MWA ablation, which were not present in simulation, suggesting inaccuracies in dielectric properties. The measured SAR may be used in simplified computer simulations to predict tissue temperature when the antenna geometry is unknown.
对于微波消融(MWA)的计算模型,了解天线设计是必要的,但临床应用器的专有设计通常是未知的。我们通过实验表征了MWA过程中的比吸收率(SAR),并与多物理场模拟进行了比较。
使用红外(IR)相机在离体肝脏模型中测量MWA过程中的SAR。将Perseon Medical的短尖端(ST)或长尖端(LT)MWA天线放置在组织样本顶部(n = 6),施加微波功率(15 W)6分钟,同时间歇性中断功率。通过红外相机记录组织表面温度(3.3帧/秒,320×240分辨率)。根据功率中断前后的温度斜率间歇性计算SAR。将温度和SAR数据与模拟结果进行比较。
一旦组织温度超过100°C,实验测量的SAR发生了相当大的变化,这与模拟结果相反。模拟和实验的消融区直径分别为横向1.28 cm和1.30±0.03 cm,轴向2.10 cm和2.66±0.22 cm。模拟和实验之间的平均温度差分别为5.6°C(ST)和6.2°C(LT)。1000 W/kg SAR等轮廓线的骰子系数分别为0.74±0.01(ST)和0.77(±0.03)(LT),表明SAR轮廓线具有良好的一致性。
我们通过实验证明了MWA消融过程中SAR的变化,这在模拟中不存在,表明介电特性存在不准确之处。当天线几何形状未知时,测量的SAR可用于简化的计算机模拟中以预测组织温度。