## Abstract The design of a cavity resonator implies to solve the Maxwell equations inside that cavity, respecting the boundary conditions. As a consequence, the resonance frequencies appear as conditions in the solutions of the differential equation involved. The measurement of the complex permitt
Resonant cavity for the measurement of microwave magnetic permeability using the small perturbation theory
β Scribed by D. X. Gouveia; L. C. Costa; M. A. Valente
- Publisher
- John Wiley and Sons
- Year
- 2008
- Tongue
- English
- Weight
- 163 KB
- Volume
- 50
- Category
- Article
- ISSN
- 0895-2477
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β¦ Synopsis
Abstract
The design of a rectangular cavity resonator implies to solve the Maxwell equations inside that cavity, respecting the boundary conditions. The resonance frequencies appear as conditions in the solutions of those equations. When a small piece of a magnetic material is introduced in the cavity, the resonance frequency and the quality factor changes. These effects can be used in the measurement of the permeability of the material. The relations are derived from the perturbation theory of resonant cavities and are simple when we consider only the firstβorder perturbation in the magnetic field caused by the sample. This is guaranteed when linearity exists between the measured perturbation and the volume of the inserted sample. In this work, a resonant cavity to measure the magnetic permeability of a material, at 2.16 GHz, was developed and characterized. Β© 2007 Wiley Periodicals, Inc. Microwave Opt Technol Lett 50: 399β402, 2008; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.23098
π SIMILAR VOLUMES
We present a new and highly stable cylindrical microwave cavity resonator designed for the measurement of the relative permittivities of gases. The cylinder has an internal volume of just 5.7 cm 3 , which makes it the smallest such a resonator reported to date. The equipment and procedure used to me
A fundamental problem in Fourier transform NMR spectroscopy is the calculation of observed resonance amplitudes for a repetitively pulsed sample, as first analyzed by Ernst and Anderson in 1966. Applications include determination of spin-lattice relaxation times (T 1 's) by progressive saturation an