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Impedance Matching (1)

Impedance Matching (1). Maximum Power Transfer. Choose an RL in order to maximize power delivered to RL. Power Delivered to the Load. Numerical Example. V TH =1 V R TH =50 Ω. Conclusion!. Maximum power is delivered to the load resistor when R L is equal to R TH.

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Impedance Matching (1)

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  1. Impedance Matching (1)

  2. Maximum Power Transfer Choose an RL in order to maximize power delivered to RL.

  3. Power Delivered to the Load

  4. Numerical Example • VTH=1 V • RTH=50 Ω

  5. Conclusion! • Maximum power is delivered to the load resistor when RL is equal to RTH.

  6. Max Power Transfer for Complex Source Impedance At resonant frequency, the series impedance of the inductor and capacitor is zero.

  7. Summary RL>RS RS>RL

  8. L Network • Different L netowrk • Difference bewteenhighpass and low pass • Examine butterworth filter from the point of view of matching….

  9. Resistance Transformation RP must be larger than RS (See derivation in the handout)

  10. Matlab Calculation

  11. Simulation Results

  12. High Pass Match Note: There is not a DC path to ZL. RS must be larger than RL! See derivation! QS=sqrt(RS/RL-1) QS=1/(ωRLC) QS=RS/(ωL)

  13. Matlab Calculation

  14. ADS Simulation

  15. Dealing With Complex Load • Absorption Approach • Resonance Technique

  16. Match Via Absorption Approach • Ignore stray component • Match the load resistance to the source resistance with an L-match • Subtract the stray component from the L-match value

  17. Absorption Example

  18. Calculation Neglecting Stray Components

  19. Account for Stray Components This technique will not work if the stray components is much larger than L match components. E.g. if 2pF is replaced by 6 pF, then this technique will not work.

  20. Resonant Approach • Resonate any stray reactance with an equal and opposite reactance at the frequency of interest!

  21. Example Resonate the 40 pF with a parallel L.

  22. Parallel Resonant Network

  23. Determine the Matching Network

  24. Resonant Approach Example

  25. Series to Parallel Conversion for RC Circuits

  26. Series to Parallel Conversion for RL Circuits

  27. Intuition • If the Q is sufficiently large, LS≈LP and CS≈CP. • RP is Q2 times RS.

  28. Summary RL>RS RS>RL

  29. Smith Chart Derivation

  30. Smith Chart Derivation (2)

  31. Smith Chart Construction (+) (-) (The center line represents an axis where X=0.)

  32. zL=1±j

  33. Adding a Series Capacitance to an Impedance

  34. Use Smith Chart Matching

  35. SmithChartMatch

  36. Smith Chart Utility 1. Select Smith Chart Match Click on Tools, then select Smith chart utility 3. Select first option

  37. Change the Load Impedance to 75 Ohms

  38. Lock Load/Source Impedance

  39. Add a Shunt Capacitance

  40. Negative Capacitance! Negative capacitance

  41. Add a Series Inductor (1) (2) Double click on the smith chart to drop the component

  42. Build ADS Circuit

  43. Comparison with Matlab Vs. ADS

  44. Adding an Inductor in Series Insertion of a series inductor to an impedance moves the impedance upward, causing a rotation clockwise along a constant circle of resistance

  45. Series Inductance Low L High L Neg L fixed frequency Insertion of a series inductor to an impedance moves the impedance upward, causing a rotation clockwise along a constant circle of resistance

  46. Adding a Capacitor in Series Insertion of a seriescapacitor to an impedance move impedance downward, causes a rotation counterclockwise along a constant circle of resistance

  47. Series Capacitance Neg C High C Low L fixed frequency Insertion of a seriescapacitor to an impedance move impedance downward, causes a rotation counterclockwise along a constant circle of resistance

  48. Admittance

  49. Admittance Example

  50. Method 1

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