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Standard Test Method for Measuring Relative Complex Permittivity and Relative Magnetic Permeability of Solid Materials at Microwave Frequencies
Automaticky přeložený název:
Standardní zkušební metoda pro měření relativní komplexní permitivity a relativní magnetickou permeabilitu pevných látek u frekvencí mikrovlnné trouby
NORMA vydána dne 15.12.2008
Označení normy: ASTM D5568-08
Poznámka: NEPLATNÁ
Datum vydání normy: 15.12.2008
Kód zboží: NS-31699
Počet stran: 8
Přibližná hmotnost: 24 g (0.05 liber)
Země: Americká technická norma
Kategorie: Technické normy ASTM
Keywords:
dielectric constant, loss factor, magnetic permeability, measurement, microwave, millimetre-wave, permittivity, radio frequency, rectangular waveguide, scattering parameter, transmission/reflection, Coaxial line, Isotropic reciprocal (non-gyromagnetic) solids, Loss index, Magnetic permeability, Microwave frequencies, Millimeter-wave, Nongyromagnetic solids, Nonmagnetic materials, Permittivity (dielectric constant)--electrical insulating materials, Radio frequency, Rectangular wave guide
| Significance and Use | ||
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Design calculations for radio frequency (RF), microwave and millimetre-wave components require the knowledge of values of complex permittivity and permeability at operating frequencies. This test method is useful for evaluating small experimental batch or continuous production materials used in electromagnetic applications. Use this method to determine complex permittivity only (in non-magnetic materials) or both complex permittivity and permeability simultaneously. |
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| 1. Scope | ||
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1.1 This test method covers a procedure for determining relative complex permittivity (relative dielectric constant and loss) and relative magnetic permeability of isotropic, reciprocal (non-gyromagnetic) solid materials. If the material is nonmagnetic, it is acceptable to use this procedure to measure permittivity only. 1.2 This measurement method is valid over a frequency range of approximately 100 MHz to over 20 GHz. These limits are not exact and depend on the size of the specimen, the size of rectangular waveguide transmission line used as a specimen holder, and on the applicable frequency range of the network analyzer used to make measurements. The practical lower and upper frequencies are limited by specimen dimension requirements (large specimens at low frequencies and small specimens at high frequencies). Being a non-resonant method, the selection of any number of discrete measurement frequencies in a measurement band would be suitable. Use of multiple rectangular waveguide transmission line sizes are required to cover this entire frequency range (100 MHz to 20 GHz). This test method can also be generally applied to circular waveguide test fixtures. The rectangular waveguide fixture is preferred over coaxial fixtures when samples have in-plane anisotropy or are difficult to manufacture precisely. 1.3 The values stated in SI units are to be regarded as the standard. The values given in parentheses are in English units. The equations shown here assume an e+jωt harmonic time convention. 1.4 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use. |
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| 2. Referenced Documents | ||
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