首页> 外文会议>IEEE/EIA International Frequency Control Symposium >DETERMINATION OF THE FREQUENCY OF OSCILLATIONS IN THE AUTODYNE'S SENSOR UNDER THE REGULAR AND CASUAL TEMPERATURE MODE VARIATIONS.
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DETERMINATION OF THE FREQUENCY OF OSCILLATIONS IN THE AUTODYNE'S SENSOR UNDER THE REGULAR AND CASUAL TEMPERATURE MODE VARIATIONS.

机译:在常规和休闲温度模式变化下,确定自动宽处传感器振荡频率的频率。

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The sensor [1] is shown on (figurel) is mounted in an orifice of the reactor wall. Antenna (2) is inward to the reactor; its conductivity depends on the permittivity of a high-temperature working body (7) and transforms to an autodyne frequency. Heating of the sensor is realized by the working body (3,4,5,) through the antenna surface. Largest part of the sensor's body is outside of the reactor and cools through the sidewalls. Variations of resonator length, permittivities of its filling, and also capacity of the diode (6) mainly influence the frequency of generation. The static temperature mode, influence to frequency variations and possible errors of the sensor value are investigated in [2]. 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 in this paper. 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 quadripole, carries out a temperature transformation into a frequency shift. Its properties are based on the wellknown thermophysics regularities. The heat exchange between working body and antenna happens by radiation under the law of Newton. 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: (1)The approximation of a temperature's curve of growth in the reactor T(t)and its Fourier-expansion (2)Determination of an impulse characteristic of 《quadripole》 h(t) in any cross-section of the sensor (3)Convolution of functions T(t) and h(t-τ)(4)Integration by the sensor's (resonator) length along a coordinate x ∈ 0, L (5)The translation into the frequency change The investigated examples have shown that the process of a sensor's warming up to stationary temperature is longer than the starting time. Frequency of generation lowering under the heating happens with a big delay, which does not enable to monitor the temperature in practical applications. Therefore, 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 is taking into account, all obtained correlations. The influence of the fluctuation's variations of temperature is considered with reference to the thermoenergetics unit, the significance of a spectral density and average quadrate of frequency fluctuations is obtained. The new theory allows measuring the temperature in the reactor with sufficient high accuracy.
机译:传感器[1]显示在(镶边)上安装在反应器壁的孔中。天线(2)向内向反应器;其电导率取决于高温工作体(7)的介电常数,并转换为自体频率。传感器的加热由工作体(3,4,5)通过天线表面实现。传感器的主体的最大部分在反应器之外,通过侧壁冷却。谐振器长度的变化,其填充的允许性,以及二极管(6)的容量主要影响产生的频率。在[2]中,研究了静态温度模式,对频率变化的影响以及传感器值可能的误差。误差,最难以补偿,是由开始时间的常规温度变化引起的。本文介绍了这种幅度的理论估计。继续调查休闲错误。传感器(具有谐振器)的工作体由线性窄带四极表示,将温度变换转换成频移。其性质基于众所周知的热物理规律。在牛顿法则下,工作体和天线之间的热交换发生。粗糙的热量导致传感器的工作体中的温度波,其具有强衰减和速度的强烈衰减,这取决于频率。数学调查包括:(1)反应器T(T)的温度的生长曲线的近似值及其傅里叶膨胀(2)在任何横截面中确定“四极”H(T)的脉冲特性的脉冲特性传感器(3)函数t(t)和h(t-t-t)的卷积(4)由传感器的(谐振器)长度沿坐标x∈0,l(5)转换为频率改变的调查示例已经表明,传感器的变暖到固定温度的过程比开始时间长。在加热下降低的发电频率随着大的延迟而发生,不会使能在实际应用中监测温度。因此,妨碍了初级和次要处理下的错误的补偿。该问题的解决方案是开发计算机模型,其考虑到所有获得的相关性。相对于热电农植物单元考虑波动的温度变化的影响,获得了光谱密度和频率波动平均四态的意义。新理论允许以足够的高精度测量反应器中的温度。

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