首页> 外文期刊>Physics in medicine and biology. >Temperature measurement errors with thermocouples inside 27 MHz current source interstitial hyperthermia applicators.
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Temperature measurement errors with thermocouples inside 27 MHz current source interstitial hyperthermia applicators.

机译:27 MHz电流源间质热敷贴器内部的热电偶的温度测量误差。

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The multielectrode current source (MECS) interstitial hyperthermia (IHT) system uses thermocouple thermometry. To obtain a homogeneous temperature distribution and to limit the number of traumas due to the implanted catheters, most catheters are used for both heating and thermometry. Implications of temperature measurement inside applicators are discussed. In particular, the impact of self-heating of both the applicator and the afterloading catheter were investigated. A one-dimensional cylindrical model was used to compute the difference between the temperature rise inside the applicators (deltaTin) and in the tissue just outside the afterloading catheter (deltaTout) as a function of power absorption in the afterloading catheter, self-heating of the applicator and the effective thermal conductivity of the surrounding tissue. Furthermore, the relative artefact (ERR), i.e. (deltaTin - deltaTout)/deltaTin, was measured in a muscle equivalent agar phantom at different positions in a dual-electrode applicator and for different catheter materials. A method to estimate the tissue temperature by power-off temperature decay measurement inside the applicator was investigated. Using clinical dual-electrode applicators in standard brachytherapy catheters in a muscle-equivalent phantom, deltaTin is typically twice as high as deltaTout. The main reason for this difference is self-heating of the thin feeder wires in the centre of the applicator. The measurement error caused by energy absorption in the afterloading catheter is small, i.e. even for materials with a high dielectric loss factor it is less than 5%. About 5 s after power has been switched off, Tin in the electrodes represents the maximum tissue temperature just before power-off. This delay time (t(delay)) and ERR are independent of Tin. However, they do depend on the thermal properties of the tissue. Therefore, ERR and t(delay) and their stability in perfused tissues have to be investigated to enable a reliable estimation of the tissue temperatures around electrodes in clinical practice.
机译:多电极电流源(MECS)间隙热疗(IHT)系统使用热电偶测温法。为了获得均匀的温度分布并限制由于植入的导管引起的外伤次数,大多数导管都用于加热和测温。讨论了施加器内部温度测量的含义。特别是,研究了涂药器和后加载导管的自热影响。一维圆柱模型用于计算涂抹器内部和后加载导管外部的组织中温度升高(δTin)之间的温差(deltaTout)作为后加载导管中功率吸收的函数,涂抹器和周围组织的有效导热率。此外,相对假象(ERR),即(δTin-δTout)/δTin,是在双电极施加器中不同位置的肌肉等效琼脂体模中以及对于不同的导管材料测量的。研究了通过施加器内部的断电温度衰减测量来估计组织温度的方法。在相当于肌肉的体模中的标准近距离放射治疗导管中使用临床双电极敷料器,deltaTin通常是delTout的两倍。造成这种差异的主要原因是涂药器中心处的细喂丝自动发热。由后加载导管中的能量吸收引起的测量误差很小,即,即使对于具有高介电损耗因子的材料,其误差也小于5%。关闭电源大约5秒钟后,电极中的锡代表刚好在关闭电源之前的最高组织温度。此延迟时间(t(delay))和ERR与Tin无关。但是,它们确实取决于组织的热特性。因此,必须研究ERR和t(delay)及其在灌注组织中的稳定性,以在临床实践中可靠地估计电极周围的组织温度。

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