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Physical Meaning of the Dipole Radiation Resistance in Lossless and Lossy Media: What is the Radiation Resistance of Antennas in Lossy Media?

机译:无损介质偶极辐射抗性的物理含义:有损媒体中天线的辐射阻力是多少?

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In this tutorial, we discuss the radiation from a Hertzian dipole into uniform isotropic lossy media of infinite extent. If the medium is lossless, the radiated power propagates to infinity, and the apparent dissipation is measured by the radiation resistance of the dipole. If the medium is lossy, the power exponentially decays, and the physical meaning of radiation resistance needs clarification. Here, we present explicit calculations of the power absorbed in the infinite lossy host space and discuss the limit of zero losses. We show that the input impedance of dipole antennas contains a radiation-resistance contribution that does not depend on the imaginary part of the refractive index. This means that the power delivered by dipole antennas to surrounding space always contains a contribution from far fields unless the real part of the refractive index is zero. Based on this understanding, we discuss the fundamental limitations of power coupling between two antennas and possibilities of removing the limit imposed by radiation damping.
机译:在本教程中,我们将从赫兹偶极子的辐射讨论为无限程度的均匀各向同性损失介质。如果介质是无损的,则辐射功率传播到无穷大,并且通过偶极子的辐射抗性测量表观耗散。如果介质有损,功率指数衰减,以及辐射抗性的物理意义需要澄清。在这里,我们在无限损耗主体空间中展示了吸收的功率的显式计算,并讨论了零损耗的极限。我们表明偶极天线的输入阻抗包含不依赖于折射率的虚部的辐射电阻贡献。这意味着偶极天线向周围空间传递的功率总是包含远场的贡献,除非折射率的实数为零。基于这种理解,我们讨论了两个天线之间的功率耦合的基本局限性以及去除辐射阻尼施加的限制的可能性。

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