Circuit Design for RF Transceivers by Domine Leenaerts, J. van der Tang, Cicero S. Vaucher

By Domine Leenaerts, J. van der Tang, Cicero S. Vaucher

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The input is short-circuited while the output is loaded by a current source. The frequency dependent voltage gain is derived RF Design: Concepts and Technology 21 as With From this expression together with the current gain expression, found to be can be where is the depletion layer capacitance of the collector-base junction. In a similar way, the can be found to be 12 where is the drain junction capacitance and the effective bulk resistance. Clearly, is more influenced by parasitic elements than and the device layout is therefore extremely important.

The dipole antenna consists of two equal arms of a certain length, configured in the same plane. 1. Let be the angle from the dipole axis for the incident electric field E. Then the effective length is defined as and the peak voltage at the terminals of the two wires is derived as follows For receive antennas, we talk about effective area instead of gain, to define the ratio of the available power to the maximum power. The available power can be derived as follows where R is the antenna resistance.

Resistances in series with the drain and source degrade the drain current and transconductance of the MOST. The source resistance will degrade the noise performance and the maximum oscillation frequency. The drain resistance will reduce the output impedance of the device. Device operations are influenced by signals on the bulk node as a result of the body effect. A proper bulk resistance network is therefore mandatory in the intrinsic device model. e. a high-ohmic or low-ohmic substrate beneath an epi layer.

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