Download e-book for iPad: Active Antennas with Non-Foster Matching Networks (Synthesis by James T. Aberle, Robert Loepsinger-Romak, Constantine A.

By James T. Aberle, Robert Loepsinger-Romak, Constantine A. Balanis

ISBN-10: 1598291025

ISBN-13: 9781598291025

Such a lot antenna engineers tend to think that antennas are one know-how that's kind of impervious to the swiftly advancing semiconductor undefined. despite the fact that, as verified during this lecture, there's a technique to include energetic elements into an antenna and remodel it right into a new type of radiating constitution that may make the most of the most recent advances in analog circuit layout. The procedure for making this modification is to use non-Foster circuit components within the matching community of the antenna. via doing so, we're now not restricted by way of the legislation of physics that follow to passive antennas. despite the fact that, we needs to now layout and build very sensitive lively circuits. This new antenna expertise is now in its infancy. The contributions of this lecture are (1) to summarize the present state of the art during this topic, and (2) to introduce a few new theoretical and functional instruments for supporting us to proceed the development of this expertise.

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Additional resources for Active Antennas with Non-Foster Matching Networks (Synthesis Lectures on Antennas)

Example text

For high frequency, internally compensated op amps such as the OPA690, the gain as a function of frequency can be represented by [12] A(s ) = A 0 ωb , s (38) where A0 represents the DC gain of the op amp and ωb represents the op amp’s 3 dB frequency. Using this gain model for the op amp, the overall transfer function T (s )of the OPA690 evaluation circuit (without the generator) can be computed (employing the golden rules of op-amps) as T (s ) = 1 ZL −Rin ZL +R − s A0 ωb 1+ Rin R . (39) It is well known that it is necessary for the poles of T (s ) to lie in the left-half of the s -plane in order for the system to be stable.

As can be seen, the −20 dB return loss bandwidth approaches 200 MHz, and the circuit is unconditionally stable at all simulation frequencies. 6 GHz. Since we are simulating our circuits below 50 MHz, we are also relying on an accurate extrapolation of the S-parameters. 9 0 0 50 100 150 200 freq, MHz (b) FIGURE 48: Simulated (a) return loss and (b) stability of the all-pass test circuit for the NE85630 FNR neglected here, but do affect the circuit performance especially stability. The simulated results for the NE85630 are the best FNR results that we obtained.

5 m A -5 V -V R R37 R=Zt Ohm VAR VAR1 Zt=5 ZL=50 CL=250 FIGURE 32: Schematic of MAX435 for simulation in Agilent ADS obtained by using the SPICE model and augmenting it to match experimental results capacitance C L and included in the analysis of the device. Ports 1 and 2 are the noninverting and inverting inputs, respectively, while ports 3 and 4 are the noninverting and inverting outputs, respectively. Included with the SPICE model are the external elements Zt, ZL , C L , and Rset along with power supply decoupling capacitors.

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Active Antennas with Non-Foster Matching Networks (Synthesis Lectures on Antennas) by James T. Aberle, Robert Loepsinger-Romak, Constantine A. Balanis


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