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Capacitor With A Dielectric01:18

Capacitor With A Dielectric

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Parallel plate capacitors consist of two conducting plates separated by a certain distance. However, it is mechanically difficult to hold the large plates parallel to each other without actual contact. Hence, a dielectric layer is commonly placed between the plates, which provides an easy solution for holding the plates together with a small gap and increases the capacitance of the capacitor.
Dielectrics are non-conducting materials with no free or loosely bound electrons. When a dielectric is...
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Gauss's Law in Dielectrics01:17

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Consider a polar dielectric placed in an external field. In such a dielectric, opposite charges on adjacent dipoles neutralize each other, such that the net charge within the dielectric is zero. When a polar dielectric is inserted in between the capacitor plates, an electric field is generated due to the presence of net charges near the edge of the dielectric and the metal plates interface. Since the external electrical field merely aligns the dipoles, the dielectric as a whole is neutral. An...
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Dielectric Polarization in a Capacitor01:31

Dielectric Polarization in a Capacitor

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The presence of a dielectric medium in a capacitor not only changes the voltage and capacitance but also affects the electric field. In general, dielectrics can be of two types: polar and nonpolar. In a polar dielectric, the positive and negative charges in the molecules are separated by a distance and hence have a permanent dipole moment. In contrast, no such charge separation exists in a nonpolar dielectric, however the nonpolar molecules get polarized in the presence of an external electric...
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Susceptibility, Permittivity and Dielectric Constant01:26

Susceptibility, Permittivity and Dielectric Constant

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When placed in an external electric field, a dielectric material gets polarized. The charge density in the dielectric material is given by the sum of the bound and free charge densities, while the total charge density can also be written in terms of the total electric field. The bound charge density can be measured in terms of polarization, leading to the relationship between electric displacement and polarization.
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Electrostatic Boundary Conditions in Dielectrics01:27

Electrostatic Boundary Conditions in Dielectrics

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When an electric field passes from one homogeneous medium to another, crossing the boundary between the two mediums imparts a discontinuity in the electric field. This results in electrostatic boundary conditions that depend on the type of mediums the field propagates through.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's permittivity....
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Targeted Cancer Therapies02:57

Targeted Cancer Therapies

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The targeted cancer therapies, also known as “molecular targeted therapies,” take advantage of the molecular and genetic differences between the cancer cells and the normal cells. It needs a thorough understanding of the cancer cells to develop drugs that can target specific molecular aspects that drive the growth, progression, and spread of cancer cells without affecting the growth and survival of other normal cells in the body.
There are several types of targeted therapies against...
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Related Experiment Video

Updated: Jan 23, 2026

Terahertz Microfluidic Sensing Using a Parallel-plate Waveguide Sensor
07:28

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A Wideband Dielectric Waveguide-Based 160-GHz Radar Target Generator.

Martin Geiger1, Christian Wegner2, Winfried Mayer3

  • 1Institute of Microwave Engineering, Ulm University, 89081 Ulm, Germany. martin-2.geiger@uni-ulm.de.

Sensors (Basel, Switzerland)
|June 26, 2019
PubMed
Summary
This summary is machine-generated.

This study introduces a low-cost dielectric waveguide radar target generator for testing radar sensors. This innovation offers a compact alternative to expensive anechoic chambers for system functionality tests.

Keywords:
dielectric waveguidedispersionfrequency-modulated continuous wave (FMCW) radarmillimeter wave radartarget generator

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Area of Science:

  • Electrical Engineering
  • Electromagnetics
  • Sensor Technology

Background:

  • Growing demand for radar sensor functionality tests in commercial and industrial applications.
  • Conventional testing relies on expensive anechoic chambers, limiting accessibility and increasing costs.
  • Need for cost-effective and compact solutions for radar sensor calibration and validation.

Purpose of the Study:

  • To present a novel, compact, and low-cost dielectric waveguide radar target generator.
  • To enable precise simulation of radar target scenarios for level probing radars.
  • To provide an alternative to traditional anechoic chamber testing methods.

Main Methods:

  • Design and simulation of a dielectric waveguide acting as a single-target scenery.
  • Manipulation of waveguide field distribution to generate specific radar reflections.
  • Full-wave simulations to design targets for realistic tank level probing scenarios.
  • Utilizing an extruded dielectric waveguide with low loss and reflection holders.

Main Results:

  • Achieved target distances ranging from 13 cm to over 9 meters using a 160 GHz dielectric waveguide.
  • Dielectric losses of 2 dB/m and low loss holders (0.5 dB) were implemented.
  • Detailed analysis of dielectric waveguide dispersion effects on frequency-modulated continuous wave (FMCW) radars.
  • Successful verification of the radar target generator with a 160 GHz FMCW radar prototype.

Conclusions:

  • The developed dielectric waveguide radar target generator is a viable, cost-effective solution for radar sensor testing.
  • The system accurately simulates realistic radar target scenarios, particularly for level probing applications.
  • This technology offers a significant advancement over conventional anechoic chamber testing, improving accessibility and reducing costs.