确定自差传感器在正常和偶然温度模式变化下的振荡频率

V.V. Boloznev, E. Safonova
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引用次数: 0

摘要

传感器安装在反应器壁的孔板上。天线向内朝向反应堆;它的电导率取决于高温工作体的介电常数,并转化为自激频率。传感器的加热是由工作体通过天线表面实现的。传感器主体的最大部分位于反应堆外部,并通过侧壁冷却。谐振腔长度、介电常数和二极管容量的变化主要影响产生频率。最难补偿的误差是由起动时的温度变化引起的。给出了这一量级的理论估计。对偶然错误的调查仍在继续。传感器的工作体(带谐振器)由线性窄带四极子表示,进行温度变换为频移。它的性质是基于众所周知的热物理规律。工作体和天线之间的热交换是通过辐射进行的。粗热在传感器的工作体中产生温度波,其传播具有很强的衰减,传播速度与频率有关。数学研究包括:(1)反应器T(T)生长温度曲线的近似及其傅里叶展开;(ii)确定传感器任意横截面上的“四极”脉冲特性h(t);(iii)函数T(T)和h(T -/spl tau/)的卷积;(iv)传感器(谐振器)长度沿坐标x/spl isin/O,L积分;(v)平移成频率变化。研究实例表明,在一次和二次处理下的误差补偿受到阻碍。解决这个问题的方法是开发一个计算机模型,它考虑了所有得到的相关性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Determination of the frequency of oscillations in the autodyne sensor under regular and casual temperature mode variations
The sensor is mounted in an orifice of the reactor wall. The antenna is inward to the reactor; its conductivity depends on the permittivity of a high-temperature working body and transforms to an autodyne frequency. Heating of the sensor is realized by the working body through the antenna surface. The largest part of the sensor's body is outside the reactor and cools through the sidewalls. Variations of resonator length, permittivities, and also capacity of the diode mainly influence the frequency of generation. The error that is most difficult to compensate for is caused by the regular temperature variations at the starting time. Theoretical estimations of this magnitude are presented. The investigation of a casual error is continued. The working body of the sensor (with a resonator), which is represented by a linear narrow-band quadrupole, carries out a temperature transformation into a frequency shift. Its properties are based on the well-known thermophysics regularities. Heat exchange between the working body and antenna occurs by radiation. The rough heat causes temperature waves in the working body of the sensor, which propagate with strong attenuation and with velocities that depend on frequency. The mathematical investigations include: (i) approximation of a temperature curve of growth in the reactor T(t) and its Fourier-expansion; (ii) determination of an impulse characteristic of "quadripole", h(t) in any cross-section of the sensor; (iii) convolution of functions T(t) and h(t-/spl tau/); (iv) integration by the sensor's (resonator) length along a coordinate x/spl isin/O,L; (v) translation into the frequency change. The investigated examples have shown that the compensation of the error under the primary and secondary processing is hampered. A solution for this problem is the development of a computer model, which takes into account all obtained correlations.
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