is measured in the same frequency band, and the third coefficient <mrow><msubsup><mi>A</mi><mn>3</mn><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msubsup></mrow> of generalised polynom <mrow><msup><mi>P</mi><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>=</mo><mstyle displaystyle="true"><mo>∑</mo><mrow><msubsup><mi>A</mi><mi>n</mi><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msubsup><mi>exp</mi><mrow><mo>(</mo><mrow><mo>−</mo><mi>j</mi><mi>n</mi><mn>2</mn><mi>π</mi><mi>f</mi><msub><mi>L</mi><mrow><mi>f</mi><mi>o</mi><mi>c</mi></mrow></msub><mo>/</mo><mi>c</mi></mrow><mo>)</mo></mrow></mrow></mstyle></mrow> is determined, which approximates the difference of measured coefficients of reflection referred to the radiator aperture: <mrow><msup><mi>P</mi><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>≈</mo><mrow><mo>(</mo><mrow><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>−</mo><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>a</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mi>exp</mi><mrow><mo>(</mo><mrow><mi>j</mi><mn>2</mn><msub><mi>φ</mi><mrow><mi>t</mi><mi>r</mi></mrow></msub><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mo>,</mo></mrow> afterwards instead of the reference reflector they install a tested reflector, the reflection coefficient is measured at the inlet of the measuring antenna <mrow><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>r</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow> in the same frequency band, and the third coefficient of the polynom <mrow><msup><mi>P</mi><mrow><mi>t</mi><mi>r</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>=</mo><mstyle displaystyle="true"><mo>∑</mo><mrow><msubsup><mi>A</mi><mi>n</mi><mrow><mi>t</mi><mi>r</mi></mrow></msubsup><mi>exp</mi><mrow><mo>(</mo><mrow><mo>−</mo><mi>j</mi><mi>n</mi><mn>2</mn><mi>π</mi><mi>f</mi><msub><mi>L</mi><mrow><mi>f</mi><mi>o</mi><mi>c</mi></mrow></msub><mo>/</mo><mi>c</mi></mrow><mo>)</mo></mrow></mrow></mstyle></mrow> is determined, which approximates difference of reflection coefficients <mrow><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>r</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>−</mo><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>a</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>,</mo></mrow> referred to the <mrow><msubsup><mi>A</mi><mn>3</mn><mi>t</mi></msubsup></mrow> radiator's aperture <mrow><msup><mi>P</mi><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>≈</mo><mrow><mo>(</mo><mrow><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>r</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>−</mo><msup><mi>S</mi><mrow><mi>t</mi><mi>a</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mi>exp</mi><mrow><mo>(</mo><mrow><mi>j</mi><mn>2</mn><msub><mi>φ</mi><mrow><mi>t</mi><mi>r</mi></mrow></msub><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mo>,</mo></mrow> the coefficient of reflection of GTR of the tested reflector is determined using the formula <mrow><msup><mi>G</mi><mrow><mi>t</mi><mi>r</mi></mrow></msup><mo>=</mo><msup><mi>G</mi><mrow><mi>r</mi><mi>e</mi><mi>t</mi></mrow></msup><mroot><mrow><mrow><mo>|</mo><mrow><msubsup><mi>A</mi><mn>3</mn><mrow><mi>t</mi><mi>r</mi></mrow></msubsup></mrow><mo>|</mo></mrow><mo>/</mo><mrow><mo>|</mo><mrow><msubsup><mi>A</mi><mn>3</mn><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msubsup></mrow><mo>|</mo></mrow></mrow><mn>3</mn></mroot><mo>.</mo></mrow> The device for measurement of the reflection coefficient comprises a metering antenna, a reference flat reflector, a device for measurement of complex amplitude of the reflected signal, a microwave cable, a calculator. At the same time the antenna is made in the form of an axisymmetric parabolic mirror with a radiator in its top, and at the edge of the mirror there is a radio transparent fixator with a mechanism of alignment of the flat reflector position.;EFFECT: higher accuracy of measurement of reflection coefficient.;2 cl, 5 dwg"/> METHOD TO MEASURE COEFFICIENT OF REFLECTION OF FLAT REFLECTOR IN MICROWAVE RANGE AND DEVICE FOR ITS REALISATION
首页> 外国专利> METHOD TO MEASURE COEFFICIENT OF REFLECTION OF FLAT REFLECTOR IN MICROWAVE RANGE AND DEVICE FOR ITS REALISATION

METHOD TO MEASURE COEFFICIENT OF REFLECTION OF FLAT REFLECTOR IN MICROWAVE RANGE AND DEVICE FOR ITS REALISATION

机译:一种在微波范围内测量平面反射镜反射系数的方法及其实现方法

摘要

FIELD: measurement equipment.;SUBSTANCE: previously calibration is performed with the help of a flat reference reflector, then perpendicularly to the axis of the mirror in the middle of the distance Lfoc between the phase centre of the radiator and the mirror focus they install a reference reflector with available coefficient of reflection of GREF, the coefficient of reflection <mrow><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow> is measured in the same frequency band, and the third coefficient <mrow><msubsup><mi>A</mi><mn>3</mn><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msubsup></mrow> of generalised polynom <mrow><msup><mi>P</mi><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>=</mo><mstyle displaystyle="true"><mo>∑</mo><mrow><msubsup><mi>A</mi><mi>n</mi><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msubsup><mi>exp</mi><mrow><mo>(</mo><mrow><mo>−</mo><mi>j</mi><mi>n</mi><mn>2</mn><mi>π</mi><mi>f</mi><msub><mi>L</mi><mrow><mi>f</mi><mi>o</mi><mi>c</mi></mrow></msub><mo>/</mo><mi>c</mi></mrow><mo>)</mo></mrow></mrow></mstyle></mrow> is determined, which approximates the difference of measured coefficients of reflection referred to the radiator aperture: <mrow><msup><mi>P</mi><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>≈</mo><mrow><mo>(</mo><mrow><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>−</mo><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>a</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mi>exp</mi><mrow><mo>(</mo><mrow><mi>j</mi><mn>2</mn><msub><mi>φ</mi><mrow><mi>t</mi><mi>r</mi></mrow></msub><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mo>,</mo></mrow> afterwards instead of the reference reflector they install a tested reflector, the reflection coefficient is measured at the inlet of the measuring antenna <mrow><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>r</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow> in the same frequency band, and the third coefficient of the polynom <mrow><msup><mi>P</mi><mrow><mi>t</mi><mi>r</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>=</mo><mstyle displaystyle="true"><mo>∑</mo><mrow><msubsup><mi>A</mi><mi>n</mi><mrow><mi>t</mi><mi>r</mi></mrow></msubsup><mi>exp</mi><mrow><mo>(</mo><mrow><mo>−</mo><mi>j</mi><mi>n</mi><mn>2</mn><mi>π</mi><mi>f</mi><msub><mi>L</mi><mrow><mi>f</mi><mi>o</mi><mi>c</mi></mrow></msub><mo>/</mo><mi>c</mi></mrow><mo>)</mo></mrow></mrow></mstyle></mrow> is determined, which approximates difference of reflection coefficients <mrow><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>r</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>−</mo><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>a</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>,</mo></mrow> referred to the <mrow><msubsup><mi>A</mi><mn>3</mn><mi>t</mi></msubsup></mrow> radiator's aperture <mrow><msup><mi>P</mi><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>≈</mo><mrow><mo>(</mo><mrow><msubsup><mi>S</mi><mrow><mn>11</mn></mrow><mrow><mi>t</mi><mi>r</mi></mrow></msubsup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow><mo>−</mo><msup><mi>S</mi><mrow><mi>t</mi><mi>a</mi></mrow></msup><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mi>exp</mi><mrow><mo>(</mo><mrow><mi>j</mi><mn>2</mn><msub><mi>φ</mi><mrow><mi>t</mi><mi>r</mi></mrow></msub><mrow><mo>(</mo><mi>f</mi><mo>)</mo></mrow></mrow><mo>)</mo></mrow><mo>,</mo></mrow> the coefficient of reflection of GTR of the tested reflector is determined using the formula <mrow><msup><mi>G</mi><mrow><mi>t</mi><mi>r</mi></mrow></msup><mo>=</mo><msup><mi>G</mi><mrow><mi>r</mi><mi>e</mi><mi>t</mi></mrow></msup><mroot><mrow><mrow><mo>|</mo><mrow><msubsup><mi>A</mi><mn>3</mn><mrow><mi>t</mi><mi>r</mi></mrow></msubsup></mrow><mo>|</mo></mrow><mo>/</mo><mrow><mo>|</mo><mrow><msubsup><mi>A</mi><mn>3</mn><mrow><mi>r</mi><mi>e</mi><mi>f</mi></mrow></msubsup></mrow><mo>|</mo></mrow></mrow><mn>3</mn></mroot><mo>.</mo></mrow> The device for measurement of the reflection coefficient comprises a metering antenna, a reference flat reflector, a device for measurement of complex amplitude of the reflected signal, a microwave cable, a calculator. At the same time the antenna is made in the form of an axisymmetric parabolic mirror with a radiator in its top, and at the edge of the mirror there is a radio transparent fixator with a mechanism of alignment of the flat reflector position.;EFFECT: higher accuracy of measurement of reflection coefficient.;2 cl, 5 dwg
机译:领域:测量设备;物质:先前的校准是在平坦的参考反射镜的帮助下进行的,然后垂直于反射镜的轴,位于镜筒相中心之间的距离L foc 的中间辐射器和反射镜焦点安装了参考反射器,其反射系数为G REF ,反射系数 <![CDATA [ S 11 r e f f ]]> <图像文件=“ 00000056.GIF” he =“ 7” imgContent =“未定义” imgFormat =“ GIF” wi =“ 14” /> 在同一频带中测量,第三个系数 <![CDATA [ A 3 r e f ]]> <图像文件=“ 00000057.GIF” he =“ 6” imgContent =“ undefined” imgFormat =“ GIF” wi =“ 8” /> 多项式 <!的形式[CDATA [ P r e f f = A n r e f exp j n 2 π f L f o c / < mi> c ]]> <图像文件=“ 00000058.GIF “ he =” 8“ imgContent =” undefined“ imgFormat =” GIF“ wi =” 70“ /> 确定,它近似于与辐射器孔径有关的反射系数的测量差: <![CDATA [ P r e f f S 11 < / mn> r e f (< / mo> f S 11 < / mn> t a f < / mi> exp j 2 φ t r < / mrow> f ]]> <图像文件=“ 00000059.GIF” he =“ 7” imgContent =“ undefined” imgFormat =“ GIF” wi =“ 82“ /> 之后,他们安装了经过测试的反射镜,而不是参考反射镜,然后在测量天线的入口处测量反射系数 <![CDATA [ S < mrow> 11 t r f ]]> <图像文件=“ 00000060.GIF” he =“ 7” imgContent =“未定义“ imgFormat =” GIF“ wi =” 12“ /> 在同一频带中,多项式的第三个系数 <![CDATA [ P t < mi> r f = A n t < / mi> r exp - < mi> j n 2 π f L f o c / c ]]> <图像文件=“ 00000061.GIF” he =“ 8” imgContent =“未定义” imgFormat =“ GIF” wi =“ 68” /> 确定,它近似反射系数的差 <![CDATA [ S 11 < mrow> t r f )< / mo> S 11 t a f < mo>, ]]> <图像文件=“ 00000062.GIF” he =“ 7” imgContent =“ undefined” imgFormat =“ GIF” wi =“ 31” /> < /数学> 引用 <![CDATA [ A 3 t ]]> <图像文件=“ 00000063.GIF” he =“ 6” imgContent =“ undefined” imgFormat =“ GIF” wi =“ 6” /> 散热器的孔 <![CDATA [ P r e f f S 11 t r f < mo>- S t a f exp j 2 φ t r f < / mrow> ]]> <图像文件=“ 00000064.GIF” he =“ 7” imgContent =“ undefined” imgFormat =“ GIF” wi =“ 81” /> 使用公式 <![CDATA [ G TR 的反射系数> t r = G r e t | < msubsup> A 3 t r < mo> | / | A 3 r e f | < / mrow> 3 ]]> <图像文件=“ 00000065.GIF” he =“ 10“ imgContent =” undefined“ imgFormat =” GIF“ wi =” 44“ /> 用于测量反射系数的设备包括:计量天线,参考平面反射器,用于测量反射信号的复振幅的设备,微波电缆,计算器。同时,天线以轴对称抛物面反射镜的形式制成,其顶部带有辐射器,并且在反射镜的边缘处有一个不透射线的固定器,其具有将平面反射器位置对齐的机制。反射系数的测量精度更高。; 2 cl,5 dwg

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