New topics: Mesh (loop) method of circuit analysis ...ee42/sp05/pdf/Week 3a.pdf · 2) Apply KVL to...
Transcript of New topics: Mesh (loop) method of circuit analysis ...ee42/sp05/pdf/Week 3a.pdf · 2) Apply KVL to...
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EECS 42, Spring 2005 Week 3a 1
Announcements
New topics:Mesh (loop) method of circuit analysisSuperposition method of circuit analysisEquivalent circuit idea (Thevenin, Norton)Maximum power transfer from a circuit to a load
To stop blowing fuses in the lab, note how the breadboards are wired …
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EECS 42, Spring 2005 Week 3a 2
Top view of board
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EECS 42, Spring 2005 Week 3a 3
Bottom view of board – note which waythe wires go
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EECS 42, Spring 2005 Week 3a 4
NODAL ANALYSIS(“Node-Voltage Method”)
0) Choose a reference node
1) Define unknown node voltages
2) Apply KCL to each unknown node, expressing current in terms of the node voltages
=> N equations forN unknown node voltages
3) Solve for node voltages=> determine branch currents
MESH ANALYSIS(“Mesh-Current Method”)
1) Select M independent mesh currents such that at least one mesh current passes through each branch*
M = #branches - #nodes + 1
2) Apply KVL to each mesh, expressing voltages in terms of mesh currents
=> M equations forM unknown mesh currents
3) Solve for mesh currents=> determine node voltages
Primary Formal Circuit Analysis Methods
*Simple method for planar circuitsA mesh current is not necessarily identified with a branch current.
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EECS 42, Spring 2005 Week 3a 5
1. Select M mesh currents.
2. Apply KVL to each mesh.
3. Solve for mesh currents.
Mesh Analysis: Example #1
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EECS 42, Spring 2005 Week 3a 6
Problem: We cannot write KVL for meshes a and b because there is no way to express the voltage drop across the current source in terms of the mesh currents.
Solution: Define a “supermesh” – a mesh which avoids the branch containing the current source. Apply KVL for this supermesh.
Mesh Analysis with a Current Source
ia ib
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EECS 42, Spring 2005 Week 3a 7
Eq’n 1: KVL for supermesh
Eq’n 2: Constraint due to current source:
Mesh Analysis: Example #2
ia ib
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EECS 42, Spring 2005 Week 3a 8
Mesh Analysis with Dependent Sources
• Exactly analogous to Node Analysis• Dependent Voltage Source: (1) Formulate and
write KVL mesh eqns. (2) Include and express dependency constraint in terms of mesh currents
• Dependent Current Source: (1) Use supermesh. (2) Include and express dependency constraint in terms of mesh currents
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EECS 42, Spring 2005 Week 3a 9
Superposition Method (Linear Circuits Only)
A linear circuit is constructed only of linear elements (linear resistors, linear dependent sources) and independent sources.
Principle of Superposition:• In any linear circuit containing multiple independent sources,
the current or voltage at any point in the network may be calculated as the algebraic sum of the individual contributions of each source acting alone.
Procedure:1. Determine contribution due to an independent source
• Set all other sources to zero (voltage source short circuit; current source open circuit)
2. Repeat for each independent source3. Sum individual contributions to obtain desired voltage or
current
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EECS 42, Spring 2005 Week 3a 10
Superposition Example• Find Vo
–+
24 V
2 Ω
4 Ω4 A
4 V+ – +
Vo
–
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EECS 42, Spring 2005 Week 3a 11
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EECS 42, Spring 2005 Week 3a 12
Lecture 6, Slide 1EECS40, Spring 2004 Prof. Sanders
Equivalent Circuit Concept• A network of voltage sources, current sources,
and resistors can be replaced by an equivalent circuit which has identical terminal properties (I-V characteristics) without affecting the operation of the rest of the circuit.
+vA_
network Aof
sourcesand
resistors
iA
?+vB_
network Bof
sourcesand
resistors
iB
iA(vA) = iB(vB)
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EECS 42, Spring 2005 Week 3a 13
• Voltage sources in series can be replaced by an equivalent voltage source:
• Current sources in parallel can be replaced by an equivalent current source:
Source Combinations
i1 i2 ≡ i1+i2
–+
–+
v1
v2
≡ –+
v1+v2
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EECS 42, Spring 2005 Week 3a 14
Thévenin Equivalent Circuit• Any* linear 2-terminal (1-port) network of indep. voltage
sources, indep. current sources, and linear resistors can be replaced by an equivalent circuit consisting of an independent voltage source in series with a resistor without affecting the operation of the rest of the circuit.
networkof
sourcesand
resistors
≡ –+
VTh
RTh
RL
iL+
vL
–
a
b
RL
iL+
vL
–
a
b
Thévenin equivalent circuit
“load” resistor
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EECS 42, Spring 2005 Week 3a 15
I-V Characteristic of Thévenin Equivalent• The I-V characteristic for the series combination of
elements is obtained by adding their voltage drops:
–+
VTh
RTh a
b
i
i
+
vab
–
v = VTh+ iR
I-V characteristic of resistor: v = iRI-V characteristic of voltage source: v = VTh
For a given current i, the voltage drop vab is equal to the sum of the voltages dropped across the source (VTh)and the across the resistor (iRTh)
v
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EECS 42, Spring 2005 Week 3a 16
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EECS 42, Spring 2005 Week 3a 17
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EECS 42, Spring 2005 Week 3a 18
Thévenin Equivalent ExampleFind the Thevenin equivalent with respect to the terminals a,b:
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EECS 42, Spring 2005 Week 3a 19
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EECS 42, Spring 2005 Week 3a 20
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EECS 42, Spring 2005 Week 3a 21
RTh Calculation Example #1
Set all independent sources to zero:
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EECS 42, Spring 2005 Week 3a 22
Comments on Dependent SourcesA dependent source establishes a voltage or current whose value depends on the value of a voltage or current at a specified location in the circuit.
(device model, used to model behavior of transistors & amplifiers)
To specify a dependent source, we must identify:1. the controlling voltage or current (must be calculated, in general)2. the relationship between the controlling voltage or current and
the supplied voltage or current3. the reference direction for the supplied voltage or current
The relationship between the dependent sourceand its reference cannot be broken!
– Dependent sources cannot be turned off for various purposes (e.g. to find the Thévenin resistance, or in analysis using Superposition).
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EECS 42, Spring 2005 Week 3a 23
RTh Calculation Example #2Find the Thevenin equivalent with respect to the terminals a,b:
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EECS 42, Spring 2005 Week 3a 24
Networks Containing Time-Varying SourcesCare must be taken in summing time-varying sources!
Example:
20 cos (100t)
1 kΩ
1 kΩ
10 sin (100t)
+
–
– +
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EECS 42, Spring 2005 Week 3a 25
Norton equivalent circuit
Norton Equivalent Circuit• Any* linear 2-terminal (1-port) network of indep. voltage
sources, indep. current sources, and linear resistors can be replaced by an equivalent circuit consisting of an independent current source in parallel with a resistor without affecting the operation of the rest of the circuit.
networkof
sourcesand
resistors
≡RL
iL+
vL
–
a
b
a
RL
iL+
vL
–iN
b
RN
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EECS 42, Spring 2005 Week 3a 26
I-V Characteristic of Norton Equivalent• The I-V characteristic for the parallel combination of
elements is obtained by adding their currents:
i
i = -IN+ Gv
I-V characteristic of resistor: i=GvI-V characteristic of current source: i = -IN
For a given voltage vab, the current i is equal to the sum of the currents in each of the two branches:
v
i+
vab
–iN
b
RN
a
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EECS 42, Spring 2005 Week 3a 27
Finding IN and RN = RTh
IN ≡ isc = VTh/RTh
Analogous to calculation of Thevenin Eq. Ckt:
1) Find open-circuit voltage and short-circuit current
2) Or, find short-circuit current and Norton (Thevenin) resistance
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EECS 42, Spring 2005 Week 3a 28
Finding IN and RN
• We can derive the Norton equivalent circuit from a Thévenin equivalent circuit simply by making a source transformation:
RLRN
iL
iN
+
vL
–
a
b
–+
RL
iL+
vL
–vTh
RTh
scTh
ThN
sc
ocThN ; i
Rvi
ivRR ====
a
b
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EECS 42, Spring 2005 Week 3a 29
Maximum Power Transfer Theorem
A resistive load receives maximum power from a circuit if the load resistance equals the Thévenin resistance of the circuit.
L
2
LTh
ThL
2L R
RRVRip ⎟⎟
⎠
⎞⎜⎜⎝
⎛+
==
–+
VTh
RTh
RL
iL+
vL
–
Thévenin equivalent circuit
( ) ( )( )
( ) ( )LTh
LThL2
LTh
4LTh
LThL2
LTh2Th
02
02
RRRRRRR
RRRRRRRV
dRdp
L
=⇒=+×−+⇒
=⎥⎦
⎤⎢⎣
⎡
++×−+
=
To find the value of RL for which p is maximum, set to 0:
Power absorbed by load resistor:
LdRdp
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EECS 42, Spring 2005 Week 3a 30