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Network Theorems
(Part II)
Dr. Mohamed Refky Amin
Electronics and Electrical Communications Engineering Department (EECE)
Cairo University
elc.n102.eng@gmail.com
http://scholar.cu.edu.eg/refky/
OUTLINE
•
•
•
•
Previously on ELCN102
Network Theorems
Norton’s Theorem
Maximum Power Transfer Theorem
2
Previously on ELCN102
Definition
Electric circuit theorems are always beneficial to help find
voltage and currents in multi loop circuits.
The network theorems include:
•
•
•
•
Superposition Theorem
Thevenin’s Theorem
Norton’s Theorem
Maximum Power Transfer Theorem
3
Previously on ELCN102
Superposition Theorem
For a linear circuit containing multiple independent sources, the
voltage across (or current through) any of its elements is the
algebraic sum of the voltages across (or currents through) that
element due to each independent source acting alone.
1.5V
𝐼a
3A
𝐼𝑏
Total
𝐼 = πΌπ‘Ž + 𝐼𝑏
4
Previously on ELCN102
Steps of Superposition Theorem
1) Keep one independent source in the circuit and turn off all
other independent sources.
2) Find the output (voltage or current) due to that active source
using one or more circuit solution methods:




Branch Method.
Simplification Method.
Loop Analysis Method.
Node Analysis Method.
3) Repeat step 1 for each of the other independent sources.
4) Find the total contribution by adding algebraically all the
contributions due to all the independent sources.
5
Previously on ELCN102
Thevenin’s Theorem
A linear two-terminal circuit, can be replaced by an equivalent
circuit consisting of a voltage source π‘‰π‘‘β„Ž in series with a resistor
π‘…π‘‘β„Ž .
6
Previously on ELCN102
Steps of Thevenin’s Theorem
1) Identify the load resistance and introduce two nodes π‘Ž and 𝑏
2) Remove the load resistance between node π‘Ž and 𝑏
3) Calculate the open circuit voltage between nodes π‘Ž and 𝑏.
This voltage is π‘‰π‘‘β„Ž of the Thevenin equivalent circuit.
4) Set all the independent sources to zero (voltage sources are
SC and current sources are OC) and calculate the resistance
seen between nodes π‘Ž and 𝑏. This resistance is π‘…π‘‘β„Ž of the
Thevenin equivalent circuit.
7
Network Theorems
Definition
Electric circuit theorems are always beneficial to help find
voltage and currents in multi loop circuits.
The network theorems include:
•
•
•
•
Superposition Theorem
Thevenin’s Theorem
Norton’s Theorem
Maximum Power Transfer Theorem
8
Norton’s Theorem
Definition
A linear two-terminal circuit can be replaced by equivalent circuit
consisting of a current source 𝐼𝑁 in parallel with a resistor 𝑅𝑁
9
Norton’s Theorem
Definition
𝐼𝑁 is the short-circuit current through nodes π‘Ž and 𝑏
10
Norton’s Theorem
Definition
𝑅𝑁 is the resistance seen between nodes π‘Ž and 𝑏 when all the
independent sources are set to zero. The same definition of 𝑹𝒕𝒉
11
Norton’s Theorem
Definition
Thevenin equivalent circuit must be equivalent to Norton
equivalent circuit
π‘‰π‘‘β„Ž
π‘‰π‘‘β„Ž
𝑅𝑁 = π‘…π‘‘β„Ž ,
π‘‰π‘‘β„Ž = 𝐼𝑁 𝑅𝑁 ,
𝐼𝑁 =
→ π‘…π‘‘β„Ž =
π‘…π‘‘β„Ž
𝐼𝑁
12
Norton’s Theorem
Solution Steps
1) Identify the load resistance and introduce two nodes π‘Ž and 𝑏
2) Remove the load resistance between node π‘Ž and 𝑏 and set all
the independent sources to zero (voltage sources are SC and
current sources are OC) and calculate the resistance seen
between nodes π‘Ž and 𝑏. This resistance is 𝑅𝑁 of the Norton
equivalent circuit.
3) Replace the load resistance with a short circuit and calculate
the short circuit current between nodes π‘Ž and 𝑏. This current
is 𝐼𝑁 of the Norton equivalent circuit.
13
Norton’s Theorem
Example (1)
Find the current in the 1𝐾٠resistor using Norton’s theorem.
14
Norton’s Theorem
Example (2)
For the shown circuit, use Norton’s theorem to find the load
current 𝐼𝐿 .
15
Network Theorems
Definition
Electric circuit theorems are always beneficial to help find
voltage and currents in multi loop circuits.
The network theorems include:
•
•
•
•
Superposition Theorem
Thevenin’s Theorem
Norton’s Theorem
Maximum Power Transfer Theorem
16
Maximum Power Transfer
Definition
The maximum amount of power will be dissipated by a load
resistance when that load resistance is equal to the
Thevenin/Norton resistance of the network supplying the power.
For maximum power 𝑃𝑅𝐿
→
𝑅𝐿 = π‘…π‘‘β„Ž = 𝑅𝑁
17
Maximum Power Transfer
Theorem Proof
𝑃𝑅𝐿 = 𝐼 2 𝑅𝐿
π‘‰π‘‘β„Ž
=
π‘…π‘‘β„Ž + 𝑅𝐿
2
= π‘‰π‘‘β„Ž
2
𝑅𝐿
𝑅𝐿
π‘…π‘‘β„Ž + 𝑅𝐿
2
For maximum power
2−2 𝑅 +𝑅 ×𝑅
𝑑𝑃𝑅𝐿
π‘‘β„Ž
𝐿
𝐿
2 1 × π‘…π‘‘β„Ž + 𝑅𝐿
= π‘‰π‘‘β„Ž
=0
𝑑𝑅𝐿
π‘…π‘‘β„Ž + 𝑅𝐿 4
18
Maximum Power Transfer
Theorem Proof
For maximum power
1 × π‘…π‘‘β„Ž + 𝑅𝐿
2
− 2 π‘…π‘‘β„Ž + 𝑅𝐿 × π‘…πΏ = 0
2
π‘…π‘‘β„Ž
+ 2π‘…π‘‘β„Ž 𝑅𝐿 + 𝑅𝐿2 − 2π‘…π‘‘β„Ž 𝑅𝐿 − 2𝑅𝐿2 = 0
2
π‘…π‘‘β„Ž
= 𝑅𝐿2
𝑅𝐿 = π‘…π‘‘β„Ž
For maximum power 𝑃𝑅𝐿
→
𝑅𝐿 = π‘…π‘‘β„Ž = 𝑅𝑁
19
Maximum Power Transfer
Power Efficiency
𝑃𝑖𝑛 = π‘ƒπ‘‰π‘‘β„Ž = π‘‰π‘‘β„Ž × πΌ
= π‘‰π‘‘β„Ž ×
π‘‰π‘‘β„Ž
π‘…π‘‘β„Ž + 𝑅𝐿
π‘ƒπ‘œπ‘’π‘‘ = 𝑃𝑅𝐿
2
= π‘‰π‘‘β„Ž
𝑅𝐿
π‘…π‘‘β„Ž + 𝑅𝐿
2
π‘ƒπ‘œπ‘’π‘‘
𝑅𝐿
× 100% =
× 100%
Power Efficiency πœ‚ =
𝑃𝑖𝑛
π‘…π‘‘β„Ž + 𝑅𝐿
20
Maximum Power Transfer
Power Efficiency
At condition of maximum power transfer (𝑅𝐿 = π‘…π‘‘β„Ž )
π‘ƒπ‘œπ‘’π‘‘ =
2
π‘‰π‘‘β„Ž
𝑅𝐿
π‘…π‘‘β„Ž + 𝑅𝐿
𝑅𝐿
πœ‚=
× 100%
π‘…π‘‘β„Ž + 𝑅𝐿
→
2
→
2
π‘‰π‘‘β„Ž
𝑅𝐿
𝑅𝐿 + 𝑅𝐿
2
2
π‘‰π‘‘β„Ž
=
4𝑅𝐿
𝑅𝐿
× 100% = 50%
𝑅𝐿 + 𝑅𝐿
21
Maximum Power Transfer
Example (3)
For the shown circuit, find the value of 𝑅𝐿 required to be
terminated between terminals π‘Ž and 𝑏 for maximum power
transfer.
22
Network Theorems
Definition
Electric circuit theorems are always beneficial to help find
voltage and currents in multi loop circuits.
The network theorems include:
•
•
•
•
Superposition Theorem
Thevenin’s Theorem
Norton’s Theorem
Maximum Power Transfer Theorem
23
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