1971
DOI: 10.1109/tim.1971.5570665
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Microwave Permittivity Measurements Using Disk Cavity Specimens

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Cited by 5 publications
(2 citation statements)
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“…As they are a priori unknown, the best possible strategy is to design the geometry of the line kept empty, in order to achieve 50 Ω. When filled lines are measured, their mismatch against 50 Ω induced by the filling powder creates the well-known ripple phenomenon [34] on the S-parameters, and so, on ε r and μ r , as they are deduced fromS-parameters using (3) and (4). Despite this ripple, the trend behavior of ε r and μ r is clearly retrieved from their mean value and further assessed by the phenomenological model (11).…”
Section: Determination Of Microwave Properties Of Nanopowdersmentioning
confidence: 99%
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“…As they are a priori unknown, the best possible strategy is to design the geometry of the line kept empty, in order to achieve 50 Ω. When filled lines are measured, their mismatch against 50 Ω induced by the filling powder creates the well-known ripple phenomenon [34] on the S-parameters, and so, on ε r and μ r , as they are deduced fromS-parameters using (3) and (4). Despite this ripple, the trend behavior of ε r and μ r is clearly retrieved from their mean value and further assessed by the phenomenological model (11).…”
Section: Determination Of Microwave Properties Of Nanopowdersmentioning
confidence: 99%
“…The test cell can be a waveguide, a coaxial line, or a planar topology. At microwaves and millimeter waves, the permittivity is derived from the measured variation of the reflection coefficient [1] at the input of a shortened waveguide [2] or a resonant cavity [3] loaded by a solid sample. For liquids or powders, transmission lines combining reflection and transmission measurements are preferred: they use waveguides or TEM (transverse electric magnetic) transmission lines, coaxial [4], or not [5,6].…”
Section: Introductionmentioning
confidence: 99%