impedance matching (1)

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Impedance Matching (1)

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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. - PowerPoint PPT Presentation

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Page 1: Impedance  Matching (1)

Impedance Matching (1)

Page 2: Impedance  Matching (1)

Maximum Power Transfer

Choose an RL in order to maximize power delivered to RL.

Page 3: Impedance  Matching (1)

Power Delivered to the Load

Page 4: Impedance  Matching (1)

Numerical Example

• VTH=1 V

• RTH=50 Ω

Page 5: Impedance  Matching (1)

Conclusion!

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

Page 6: Impedance  Matching (1)

Max Power Transfer for Complex Source Impedance

At resonant frequency, the series impedance of the inductor and capacitor is zero.

Page 7: Impedance  Matching (1)

Summary

RL>RS RS>RL

Page 8: Impedance  Matching (1)

L Network

• Different L netowrk• Difference bewteen highpass and low

pass• Examine butterworth filter from the

point of view of matching….

Page 9: Impedance  Matching (1)

Resistance Transformation

(See derivation in the handout)

RP must be larger than RS

Page 10: Impedance  Matching (1)

Matlab Calculation

Page 11: Impedance  Matching (1)

Simulation Results

Page 12: Impedance  Matching (1)

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)

Page 13: Impedance  Matching (1)

Matlab Calculation

Page 14: Impedance  Matching (1)

ADS Simulation

Page 15: Impedance  Matching (1)

Dealing With Complex Load

• Absorption Approach• Resonance Technique

Page 16: Impedance  Matching (1)

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

Page 17: Impedance  Matching (1)

Absorption Example

Page 18: Impedance  Matching (1)

Calculation Neglecting Stray Components

Page 19: Impedance  Matching (1)

Account for Stray Components

This technique will not work if the stray components is much largerthan L match components. E.g. if 2pF is replaced by 6 pF, then this technique will not work.

Page 20: Impedance  Matching (1)

Resonant Approach

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

Page 21: Impedance  Matching (1)

Example

Resonate the 40 pF with a parallel L.

Page 22: Impedance  Matching (1)

Parallel Resonant Network

Page 23: Impedance  Matching (1)

Determine the Matching Network

Page 24: Impedance  Matching (1)

Resonant Approach Example

Page 25: Impedance  Matching (1)

Series to Parallel Conversion for RC Circuits

Page 26: Impedance  Matching (1)

Series to Parallel Conversion for RL Circuits

Page 27: Impedance  Matching (1)

Intuition

• If the Q is sufficiently large, LS≈LP and CS ≈CP.

• RP is Q2 times RS.

Page 28: Impedance  Matching (1)

Summary

RL>RS RS>RL

Page 29: Impedance  Matching (1)

Smith Chart Derivation

Page 30: Impedance  Matching (1)

Smith Chart Derivation (2)

Page 31: Impedance  Matching (1)

Smith Chart Construction

(The center line represents an axis where X=0.)

(+)

(-)

Page 32: Impedance  Matching (1)

zL=1±j

Page 33: Impedance  Matching (1)

Adding a Series Capacitance to an Impedance

Page 34: Impedance  Matching (1)

Use Smith Chart Matching

Page 35: Impedance  Matching (1)

SmithChartMatch

Page 36: Impedance  Matching (1)

Smith Chart Utility1. Select Smith Chart Match2. Click on Tools, then select Smith chart utility3. Select first option

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Change the Load Impedance to 75 Ohms

Page 38: Impedance  Matching (1)

Lock Load/Source Impedance

Page 39: Impedance  Matching (1)

Add a Shunt Capacitance

Page 40: Impedance  Matching (1)

Negative Capacitance!

Negative capacitance

Page 41: Impedance  Matching (1)

Add a Series Inductor

(1)

(2)

Double click on the smith chart to drop the component

Page 42: Impedance  Matching (1)

Build ADS Circuit

Page 43: Impedance  Matching (1)

Comparison with Matlab Vs. ADS

ADS Matlab

Shunt Cap 1.511 pF 1.5 pF

Series L 5.72 nH 5.627 nH

Page 44: Impedance  Matching (1)

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

Page 45: Impedance  Matching (1)

Series Inductance

Neg L

High LLow 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

Page 46: Impedance  Matching (1)

Adding a Capacitor in Series

Insertion of a series capacitor to an impedance move impedance downward, causes a rotation counter clockwise along a constant circle of resistance

Page 47: Impedance  Matching (1)

Series Capacitance

High C Low L

Neg C

fixed frequency

Insertion of a series capacitor to an impedance move impedance downward, causes a rotation counter clockwise along a constant circle of resistance

Page 48: Impedance  Matching (1)

Admittance

Page 49: Impedance  Matching (1)

Admittance Example

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Method 1

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Method 2

1. Find the Z.2. Rotate Smith Chart 180 degrees

Page 52: Impedance  Matching (1)

Smith Chart Construction

(The center line represents an axis where X=0.)

(+)

(-)Conductancecircle

Inductive susceptance

Rotate the impedance chart by 180 degrees

Capacitive susceptance

Page 53: Impedance  Matching (1)

Enable Admittance Chart

Page 54: Impedance  Matching (1)

Adding a Shunt Capacitance

Insertion of a shunt capacitor causes a rotation clockwise along a constant circle of admittance

Page 55: Impedance  Matching (1)

Adding a Shunt Capacitance

High C Low C

Neg C

fixed frequency

Insertion of a shunt capacitor causes a rotation clockwise along a constant circle of admittance

Page 56: Impedance  Matching (1)

Adding a Shunt Inductance

Insertion of a shunt inductor causes a rotation counter clockwise along a constant circle of admittance

Page 57: Impedance  Matching (1)

Shunt Inductance

Neg Ind

High LLow L

fixed frequency

Insertion of a shunt inductor causes a rotation counter clockwise along a constant circle of admittance

Page 58: Impedance  Matching (1)

Next Class

• Pi Network• T Network• Smith Chart• Genesis

Page 59: Impedance  Matching (1)

The Pi Network

The virtual resistance must be less than RS and RL.