1994
DOI: 10.1109/22.330113
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A microstrip phase-trim device using a dielectric overlay

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Cited by 20 publications
(29 citation statements)
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“…As said before, to the authors' best knowledge, the only analytical formula already presented in the literature for the effective permittivity (and, thus, for the characteristic impedance) of a covered microstrip line is the one reported in Gouker and Kushner (1996). Such a formula is effective only in a certain range of the physical parameters describing the structure (see formulas 5(a) and (b) in Gouker and Kushner (1996)). Specifically, the ratio between the relative permittivity of the cover and of the substrate should not exceed four and the normalized width of the strip should not exceed 12= ffiffiffiffi ffi 1 r p .…”
Section: Numerical Resultsmentioning
confidence: 99%
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“…As said before, to the authors' best knowledge, the only analytical formula already presented in the literature for the effective permittivity (and, thus, for the characteristic impedance) of a covered microstrip line is the one reported in Gouker and Kushner (1996). Such a formula is effective only in a certain range of the physical parameters describing the structure (see formulas 5(a) and (b) in Gouker and Kushner (1996)). Specifically, the ratio between the relative permittivity of the cover and of the substrate should not exceed four and the normalized width of the strip should not exceed 12= ffiffiffiffi ffi 1 r p .…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Assuming a quasi-TEM propagating mode, the characteristic impedance can be expressed as Z 0 ¼ Z 0; air = ffiffiffiffiffiffiffi 1 eff r q (Gouker and Kushner, 1996), where Z 0,air is the COMPEL 32,6 characteristic impedance of an air-loaded microstrip line (i.e. substrate permittivity is equal to 1 0 ), 1 eff r is the effective relative permittivity given by 1 eff r ¼ C=C air , C is the per unit length capacitance of the line of Figure 1 and C air is the per unit length capacitance of an air loaded line with the same geometry.…”
Section: Theorymentioning
confidence: 99%
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“…The leaves have complex dielectric constant, with the real part depending on the phase and the imaginary part on the amplitude change. Since our experimental data gave only the amplitude change, the formula suggested by Gouker and Kushner [1994] was used to calculate the phase change due to overlay. The amount of phase trim (in degrees) for a particular overlay is given by…”
Section: Effect Of Acalypha (Ac)mentioning
confidence: 99%