22nd European Microwave Conference, 1992 1992
DOI: 10.1109/euma.1992.335735
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Resistive Sensors for High Pulse Power Microwave Measurements

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Cited by 8 publications
(8 citation statements)
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“…If the longitudinal axis of the horn antenna is adjusted to be parallel to the mw power flux, the mw power getting into waveguide P can be obtained from the following expression P=Wp11s' (1) where Wp is the mw power flow density (Pounting's vector) in a free space, 1 is the efficiency and S is the cross-sectional area of the horn antenna. We have measured the mw pulse power P getting into waveguide when the receiving horn antenna is placed at a distance L from the transmitting one.…”
Section: Resultsmentioning
confidence: 99%
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“…If the longitudinal axis of the horn antenna is adjusted to be parallel to the mw power flux, the mw power getting into waveguide P can be obtained from the following expression P=Wp11s' (1) where Wp is the mw power flow density (Pounting's vector) in a free space, 1 is the efficiency and S is the cross-sectional area of the horn antenna. We have measured the mw pulse power P getting into waveguide when the receiving horn antenna is placed at a distance L from the transmitting one.…”
Section: Resultsmentioning
confidence: 99%
“…As it was shown by Baltusis et al (1), one of the most perspective devices for high microwave pulsed power measurement are resistive heads, where a resistive sensor made from n-type Si is used as a sensitive element. The performance of the resistive sensor is based on the semiconductor resistance change due to the electron heating effect.…”
Section: Operation Of the Resistive Headmentioning
confidence: 99%
“…The sample is inserted in the centre of the double ridged waveguide and covers the gap region of it. It is analogous to the crosswaveguide type RS in a rectangular waveguide demonstrating high sensitivity and flat frequency response [2]. These facts stimulated our investigations with a purpose to find a more acceptable layout of the SE for the measurement of microwave pulse power propagating in a double ridged waveguide.…”
Section: Introductionmentioning
confidence: 99%
“…The power flow in the waveguide at finite frequency can be expressed in terms of the power flow at infinite frequency: (2) where λ is the wavelength of electromagnetic wave in free space. As it was shown in [12] P ∞ can be expressed as follows: (3) where E 0 is an amplitude of electric field in the centre of the empty waveguide, Z 0 is an impedance of free space, and the rest parameters in Eq.…”
Section: Double Ridged Waveguidementioning
confidence: 99%
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