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Determining the complex permittivity and the complex permeability of magnetodielectric materials in the range of centimeter and decimeter waves

机译:在厘米和减距波浪范围内测定磁电材料的复杂介电常数和复合渗透率

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The relatively simple measuring methods for determinign the comple xpermittivity and the complex permeability of magnetodielectric materials are presented. Measurements must be done with each sample of any magnetodielectric by two methods: the short circuit metod and the idling method. For measurements by the short circuit method, a magnetodielectric sample is placed in the measuring waveguide near the short circuit end. For measurements by the idling method, a magnetodielectric sample is placed in the measuring waveguide at a quarter of the wavelength distance from the short circuit end. The measurements are taken equally for both methods. The measuring waveguide (with a sample) is connected to the standard measuring line. the other end of the measuring line is connected to a transmitter. A transmitter radiates waves of a given frequency, they are reflected by the short circuit end of a measuring waveguide containing a magnetodielectric sample and standing waves are set up Standing wave parameters can be measured by the standard measuring line and the indicator. The coefficient of the stading wave 1/ k and the displacement triangle openx of a minimum of the electric field intensity (due to decrease of the wavelength in a magnetodielectric sample) are measured by short circuit and idling methods. Both methods lead to the transcendental equaton which determines the complex wave propagation coefficient in a magnetodielectric sample as a function of a sample thickness, the wavelength, 1/k and triangle openx from both measuring methods. After that the complex permeability of the under investigation magnetodielectric is taken as a function of the complex wave propagation coefficient, a sample thickness, the wavelength, 1/k and triangle openx from both measuring methods. The complex permittivity of this magnetodielectric is taken as a function of the complex wave propagation coefficient, a thickness of a sample, the wavelength and the complex permeability.
机译:介绍了用于确定氧化物氧化性积水的相对简单的测量方法和磁电极材料的复杂渗透率。必须通过两种方法使用任何磁电电电二电电的每个样本进行测量:短路式测量和空转方法。为了通过短路方法进行测量,将磁电电电样品放置在短路端附近的测量波导中。为了通过空转方法测量,将磁电测量放置在距短路端的波长距离的四分之一的测量波导中。两种方法都同样地进行测量。测量波导(带样品)连接到标准测量线。测量线的另一端连接到发射器。发射器辐射给定频率的波,它们由包含磁电测量的测量波导的短路端反射,驻波设置驻波参数可以通过标准测量线和指示器测量。通过短路和怠速方法测量体场强度的最小电场强度(由于波长在磁电测量中的波长)的最小电场强度(由于波长)的置换三角形的系数。这两种方法都导致了超恒定的方案,其根据来自两个测量方法的样品厚度,波长,1 / k和三角形Openx的函数确定磁电电极样品中的复杂波传播系数。之后,在来自两个测量方法的复杂波传播系数,样品厚度,波长,1 / k和三角形OpenX的函数中,将磁力电压的复杂渗透率作为复杂波传播系数,样品厚度,波长,1 / k和三角形OpenX。这种磁电极的复杂介电常数是复杂波传播系数的函数,样品的厚度,波长和复杂渗透率的函数。

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