An Iterative Electro-Thermal Model for an Active Antenna Element and its Application to Arrays

Conference Paper (2025)
Author(s)

F.T. Çelik (TU Delft - Microwave Sensing, Signals & Systems)

C Fager (Chalmers University of Technology)

Alexander Yarovoy (TU Delft - Microwave Sensing, Signals & Systems)

Y. Aslan (TU Delft - Microwave Sensing, Signals & Systems)

Microwave Sensing, Signals & Systems
DOI related publication
https://doi.org/10.23919/EuMC65286.2025.11235236
More Info
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Publication Year
2025
Language
English
Microwave Sensing, Signals & Systems
Bibliographical Note
Green Open Access added to TU Delft Institutional Repository as part of the Taverne amendment. More information about this copyright law amendment can be found at https://www.openaccess.nl. Otherwise as indicated in the copyright section: the publisher is the copyright holder of this work and the author uses the Dutch legislation to make this work public.@en
Pages (from-to)
1127-1130
ISBN (print)
979-8-3315-1260-6
ISBN (electronic)
978-2-87487-081-1
Reuse Rights

Other than for strictly personal use, it is not permitted to download, forward or distribute the text or part of it, without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license such as Creative Commons.

Abstract

A novel electro-thermal model at the unit-cell level for active phased arrays is proposed to establish a link between the power amplifier (PA) output signal and its junction temperature. The iterative model is developed in four stages: (i) calculation of the PA output, (ii) computation of the dissipated power of the PA, (iii) thermal simulation for temperature assessment, and (iv) update on the PA output with the new temperature. These steps are repeated until the PA temperature is convergent. The use of the model is demonstrated with an amplitude-tapered 16-element array of single-stage class-A amplifier and patch antenna unit-cells at 2.14 GHz. It is observed that the inclusion of the temperature effects in the array pattern causes around a 2 dB drop in the radiated power, while the peak side lobe level (SLL) increases by up to 7.75 dB for 40 dB Taylor tapering.

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