1 / 10

Lecture 14 RLC Resonators with TEM feed & TEM Resonators

Lecture 14 RLC Resonators with TEM feed & TEM Resonators. 6.013. ELECTROMAGNETICS AND APPLICATIONS. Luca Daniel. Outline. Review of Fundamental Electromagnetic Laws Electromagnetic Waves in Media and Interfaces Digital & Analog Communications

phila
Télécharger la présentation

Lecture 14 RLC Resonators with TEM feed & TEM Resonators

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Lecture 14RLC Resonators with TEM feed& TEM Resonators 6.013 ELECTROMAGNETICS AND APPLICATIONS Luca Daniel

  2. Outline • Review of Fundamental Electromagnetic Laws • Electromagnetic Waves in Media and Interfaces • Digital & Analog Communications • TEM transmission lines (cables and IC/PCB traces) • Digital communications (transients) • RF communications (matching loads to amplifiers) • RLC resonators (application: e.g. filters) • RLC resonators • Matching (Coupling to) RLC resonators • RLC resonators with TEM feed • Examples: cellphone channel selection filter. Notch filter. • TEM resonators • Half-wave and quarter-wave resonators • Quality factor of TEM resonators • Coupling to TEM resonators Today

  3. Power Delivery (Coupling) to RLC Resonators I(w) Ri Power delivered into series resonator Ri : PDi() RS L + VS - C To maximize PDi choose: to maximize power delivery: drive at resonance frequency! 1 Dw Half-power bandwidth: 1/2 w wo If Rs is given, to maximize PDi choose Ri s.t.: Critically Matched! For critically matched resonator:

  4. RLC resonators with TEM feed Ri + G L Zo =RS G Zo =RS L C - Ri C Behavior at resonance: 0 if critically matched (Ri=Z0) 1 if Ri=0/∞ (short/open) circuit Behavior away from resonance: Series resonance: Open circuit Parallel resonance: Short circuit

  5. Example #1 – Cell Phone Filter (band-pass) RS + G L Zo =RS C Vs - Ri Cell phone (band-pass filter) specifications for channel selection: - Looks like a short circuit far from channel frequency (reflects all power) - At channel freq reflect < 1/9 of the incident power (want max coupling) - channel frequency = 1 GHz - bandwidth = 10 MHz - available amplifier has RS = 100-ohm Filter solution: Parallel resonators look like short circuits far from o Small, hard to build, use TEM?

  6. Zo L Zo R VTh C Example #2 – Notch Filter (i.e. interference suppression) Notch (band-stop) filter specs for suppression of interfering channel: Far from wo the load is matched (signal goes to amplifier R) At wo reflect all incident power; let G = -1 (short circuit) wo = 2 106 Dw = 2  104 (rejected band, notch filter) Zo = 100-ohm line Filter solution: Lossless series resonators look like short circuits at wo

  7. Outline • Review of Fundamental Electromagnetic Laws • Electromagnetic Waves in Media and Interfaces • Digital & Analog Communications • TEM transmission lines (cables and IC/PCB traces) • Digital communications (transients) • RF communications (matching loads to amplifiers) • RLC resonators (application: e.g. filters) • RLC resonators • Matching (Coupling to) RLC resonators • RLC resonators with TEM feed • Examples: cellphone channel selection filter. Notch filter. • TEM resonators • Half-wave and quarter-wave resonators • Quality factor of TEM resonators • Coupling to TEM resonators Today

  8. Standing Waves on Shorted TEM Line c c Every half wavelength the TEM line behaves like a short circuit! z

  9. Open and Short Circuit “Half-Wave” TEM Resonators i + v Zo, n - D Short-Circuit Resonator: z i + v Zo, n - D v(z,t) Z0 i(t,z) case: n=2 z 0 D Open-Circuit Resonator: v(z,t) Z0 i(t,z) z D 0 case: n=2

  10. “Quarter-Wave” TEM Resonators E.g. Short-Open Resonator: i + v Zo, n - D v(z,t) Z0 i(t,z) 1 2 z 0 D D = l/4, 3l/4, 5l/4,… = (ln/4)(2n - 1)

More Related