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Lecture 22 1 Series and Parallel Resistors/Impedances
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Page 1: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 1

Series and Parallel Resistors/Impedances

Page 2: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 2

Introduction

• For analysis, series resistors/impedances can be replaced by an equivalent resistor/ impedance.

• Parallel resistors/impedances can be replaced by an equivalent resistor/ impedance.

Page 3: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 3

Introduction

• Complicated networks of resistors/ impedances can be replaced by a single equivalent resistor/impedance.

Page 4: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 4

Equivalent Resistancei(t)

+

-

v(t)

i(t)

+

-

v(t)Req

Req is equivalent to the resistor network on the left in the sense that they have the same i-v characteristics.

Page 5: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 5

Equivalent Resistance

• The rest of the circuit cannot tell whether the resistor network or the equivalent resistor is connected to it.

• The equivalent resistance cannot be used to find voltages or currents internal to the resistor network.

Page 6: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 6

Equivalent ImpedanceI

+

-

V

I

+

-

VZeq

Zeq is equivalent to the network on the left in the sense that they have the same phasor I-V characteristics at the frequency .

Page 7: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 7

Series Resistance

R1

R3

R2 Req

Req = R1 + R2 + R3

Page 8: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 8

Series

Two elements are in series if the current that flows through one must also flow through the other.

R1 R2

Series

R1 R2

Not Series

Page 9: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 9

Zeq

Series Impedance

Z1

Zeq = Z1 + Z2 + Z3

Z3

Z2

Page 10: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 10

Example: Series Inductors

• What is the equivalent impedance of two series inductors?

L2L1

Page 11: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 11

Series Inductors

• The equivalent impedance is

j(L1+L2)

• Two inductors in series are equivalent to a single inductor whose inductance is the sum of the two inductances.

Page 12: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 12

Parallel Resistance

Req

1/Req = 1/R1 + 1/R2 + 1/R3

R3R2R1

Page 13: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 13

Parallel

Two elements are in parallel if they are connected between the same two nodes.

Parallel

Not Parallel

R1

R2

R1

R2

Page 14: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 14

Parallel Impedance

1/Zeq = 1/Z1 + 1/Z2 + 1/Z3

Z3Z1 Z2 Zeq

Page 15: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 15

Example: Parallel Capacitors

• What is the equivalent impedance of two parallel capacitors?

C1 C2

Page 16: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 16

Parallel Capacitors

• The equivalent impedance is

• Two capacitors in parallel are equivalent to a single capacitor whose capacitance is the sum of the two capacitances.

21

1

CCj

Page 17: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 17

Example: Ladder Network

• Ladder networks are used in analog-to-digital converters to provide reference voltages that are 1/2, 1/4, 1/8, etc. of a source voltage.

Page 18: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 18

Ladder Network

1k

1k

2k

1k

2k

Find the equivalent resistance.

Page 19: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 19

Ladder Network

Find the equivalent resistance by making combinations of series and parallel resistors until you have only one resistor left.

Page 20: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 20

Ladder Network

2k2k

1k

2k

Page 21: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 21

Ladder Network

1k

1k

2k

Page 22: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 22

Ladder Network

2k2k

Page 23: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 23

Ladder Network

1k

The equivalent resistance of the ladder network is 1k

Page 24: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 24

10

769pF

159H

Bandpass Filter

For = 2.86 106, find the equivalent impedance.

Page 25: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 25

10

-j455

j455

Compute Impedances

Now combine series impedances

Page 26: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 26

-j45510 j455

Bandpass Filter

Now combine parallel impedances

455.1 88.7

Page 27: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 27

Bandpass Filter

3.1k7.2045510455

45510455

jj

jj

Page 28: Lecture 221 Series and Parallel Resistors/Impedances.

Lecture 22 28

Loaded Bandpass Filter

For = 2.86 106, find the equivalent impedance.

10

769pF

159H

50k