Transcript EE2003 Circuit Theory

電路學(一)
Chapter 4
Circuit Theorems
1
Circuit Theorems - Chapter 4
4.1
4.2
4.3
4.4
4.5
4.6
4.7
Motivation
Linearity Property
Superposition
Source Transformation
Thevenin’s Theorem
Norton’s Theorem
Maximum Power Transfer
2
4.1 Motivation (1)
If you are given the following circuit, are
there any other alternative(s) to determine
the voltage across 2W resistor?
What are they? And how?
Can you work it out by inspection?
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4.2 Linearity Property (1)
It is the property of an element describing a linear relationship
between cause and effect(因果線性關係).
A linear circuit is one whose output is linearly related (or
directly proportional) to its input.
Homogeneity (scaling) property
v=iR
→
kv=kiR
Additive property
v1 = i1 R and v2 = i2 R
→
v = (i1 + i2) R = v1 + v2
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4.2 Linearity Property (2)
Example 1
Find Io when vs =12 V and vs =24 V .
(p.129)
3vx
4.2 Linearity Property (2)
Example 2
By assume Io = 1 A, use linearity to find the actual value of Io in the
circuit shown below.
(p.130)
*Refer to in-class illustration, text book, answer Io = 3A
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4.3 Superposition Theorem(重疊原理) (1)
It states that the voltage across(端電壓) (or current
through) an element in a linear circuit is the
algebraic sum of the voltage across (or currents
through) that element due to EACH independent
source acting alone.
The principle of superposition helps us to analyze
a linear circuit with more than one independent
source by calculating the contribution of each
independent source separately.
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4.3 Superposition Theorem(重疊原理) (2)
We consider the effects of 8A and 20V one
by one, then add the two effects together
for final vo.
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4.3 Superposition Theorem(重疊原理) (3)
Steps to apply superposition principle
1. Turn off all independent sources except one
source. Find the output (voltage or current)
due to that active source using nodal or
mesh analysis.
2. Repeat step 1 for each of the other independent
sources.
3. Find the total contribution by adding
algebraically all the contributions due to the
independent sources.
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4.3 Superposition Theorem(重疊原理) (4)
Two things have to be keep in mind:
1. When we say turn off all other independent
sources:
 Independent voltage sources are replaced
by 0 V (short circuit短路) and
 Independent current sources are replaced
by 0 A (open circuit開路).
2. Dependent sources are left intact because
they are controlled by circuit variables.
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4.3 Superposition Theorem(重疊原理) (5)
Example 3
Use the superposition theorem to find
v in the circuit shown below.
(p.131)
3A is discarded
by open-circuit
6V is discarded
by short-circuit
*Refer to in-class illustration, text book, answer v = 10V
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4.3 Superposition Theorem(重疊原理) (6)
Example 4
Find i0 in the circuit using the superposition.
(p.132)
2W
3W
1W
5i0
+–
i0
4W
4A
5W
+–
20 V
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4.3 Superposition Theorem(重疊原理) (7)
Example 5
Use superposition to find vx in
the circuit below.
(p.134)
2A is discarded by
open-circuit
20 W
10 V
10V is discarded
by open-circuit
20 W
v1
+

4W
(a)
0.1v1
Dependant source
keep unchanged
v2
2A
4W
0.1v2
(b)
*Refer to in-class illustration, text book, answer vx = 12.5V
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4.4 Source Transformation(電源轉換) (1)
• An equivalent circuit is one whose v-i
characteristics are identical with the
original circuit.
• It is the process of replacing a voltage
source vS in series with a resistor R by a
current source iS in parallel with a resistor
R, or vice versa.
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4.4 Source Transformation(電源轉換) (2)
+
+
-
-
+
+
-
-
(a) Independent source transform
(b) Dependent source transform
• The arrow of the
current source is
directed toward
the positive
terminal of the
voltage source.
• The source
transformation is
not possible when
R = 0 for voltage
source and R = ∞
for current source.
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4.4 Source Transformation(電源轉換) (3)
Example 6
Find io in the circuit shown below using source transformation.
(p.137)
*Refer to in-class illustration, textbook, answer io = 1.78A
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4.4 Source Transformation(電源轉換) (4)
Example 7
Find vx in the circuit shown below using source transformation.
(p.138)
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4.5 Thevenin’s Theorem(戴維寧定理) (1)
It states that a linear two-terminal
circuit (Fig. a) can be replaced by an
equivalent circuit (Fig. b) consisting
of a voltage source VTH in series with
a resistor RTH,
where
• VTH is the open-circuit voltage at the
terminals.
• RTH is the input or equivalent resistance at
the terminals when the independent
sources are turned off.
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4.5 Thevenin’s Theorem(戴維寧定理) (2)
Example 8
Find the Thevenin’s equivalent circuit to the left of the
terminals a-b. Then find the current through RL =6, 16,
and 36 W
(p.140)
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4.5 Thevenin’s Theorem(戴維寧定理) (3)
Example 9
Using Thevenin’s theorem, find
the equivalent circuit to the left
of the terminals in the circuit
shown below. Hence find i.
(p.142)
6W
6W
4W
RTh
(a)
6W
2A
6W
2A
+
VT
4W
h

(b)
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*Refer to in-class illustration, textbook, answer VTH = 6V, RTH = 3W, i = 1.5A
4.5 Thevenin’s Theorem(戴維寧定理) (4)
Example 10
Find the Thevenin’s equivalent of the circuit at terminal a-b.
(p.142)
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4.5 Thevenin’s Theorem(戴維寧定理) (5)
Example 11
Find the Thevenin equivalent
circuit of the circuit shown
below to the left of the
terminals.
(p.143)
5W
+

6V
3W
Ix
a
+
VTh
4W 
i2
i1
1.5Ix
i2
i1
o
b
(a)
0.5I
3W
x
5W
1.5Ix
(b)
Ix
i
a
+ 1V

4W
b
*Refer to in-class illustration, textbook, answer VTH = 5.33 V, RTH = 0.44 W
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4.5 Thevenin’s Theorem(戴維寧定理) (6)
Example 12
Determine the Thevenin equivalent of the circuit
shown below at terminals a-b.
(p.143)
4.6 Norton’s Theorem(諾頓定理) (1)
It states that a linear two-terminal circuit
can be replaced by an equivalent circuit
of a current source IN in parallel with a
resistor RN,
Where
• IN is the short circuit current through
the terminals.
• RN is the input or equivalent resistance
at the terminals when the independent
sources are turned off.
The Thevenin’s and Norton equivalent circuits are
related by a source transformation.
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4.6 Norton’s Theorem(諾頓定理) (2)
Example 13
Find the Norton equivalent
circuit of the circuit shown
below.
(p.148)
2vx
i
+ 
+
vx

6W
2W
ix
+
vx

1V
+

(a)
2vx
+ 
6W
2W
10 A
+
vx

Isc
(b)
*Refer to in-class illustration, textbook, RN = 1W, IN = 10A.
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4.7 Derivation of Thevenin’s and
Norton’s Theorems (1)
Suppose the linear circuit contains
two independent voltage sources vs1
and vs2 and two independent current
sources is1 and is2
v  A0i  A1vs1  A2vs2  A 3is1  A4is2
v  A0i  B0
4.8 Maximum Power Transfer
(最大功率傳輸定理) (1)
If the entire circuit is replaced by
its Thevenin equivalent except for
the load, the power delivered to
the load is:
2
 VTh 
 RL
P  i 2 RL  
 RTh  RL 
For maximum power dissipated
in RL, Pmax, for a given RTH,
and VTH,
2
RL  RTH

Pmax
V
 Th
4 RL
The power transfer profile with
different RL
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4.8 Maximum Power Transfer
(最大功率傳輸定理) (2)
Example 14
Determine the value of RL that will
draw the maximum power from
the rest of the circuit shown below.
Calculate the maximum power.
+
vx
4W
v0
+
i
2W
vx
4W

Fig. a
2W
1W
1W
+

+

3vx
(a)
1V
+

9V
io
+

3vx
+
VTh

=> To determine RTH
Fig. b
=> To determine VTH
(b)
*Refer to in-class illustration, textbook, RL = 4.22W, Pm = 2.901W
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4.9 Applications (1)
4.9 Applications (2)
Example 16
The terminal voltage of a voltage source is 12 V when
connected to a 2-W load. When the load is disconnected,
the terminal voltage rises to 12.4 V. (a) Calculate the
source voltage vs and internal resistance Rs. (b)
Determine the voltage when an 8-W load is connected to
the source.
(p.157)
4.9 Applications (3)
R3
Rx 
R2
R1
The Wheatstone bridge
4.9 Applications (4)
Example 17
The circuit represents an unbalanced bridge. If the
galvanometer has a resistance of 40 W, find the current
through the galvanometer.
(p.159)