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Cheatsheet: Network Theorems

1. Superposition Theorem

1.1 Principle

ConceptDescription
StatementIn a linear circuit with multiple independent sources, the voltage or current in any element equals the algebraic sum of voltages or currents produced by each source acting independently
Linearity RequirementApplies only to linear circuits; all resistors, capacitors, inductors must have constant values
Source DeactivationVoltage sources → short circuit (0 V); Current sources → open circuit (0 A)

1.2 Procedure

  • Deactivate all independent sources except one
  • Calculate the desired voltage or current due to that single source
  • Repeat for each independent source individually
  • Algebraically sum all individual responses (consider polarity/direction)
  • Dependent sources remain active throughout all calculations

1.3 Power Calculation

  • Cannot apply superposition directly to power (nonlinear relationship: P = I²R or P = V²/R)
  • Calculate total voltage or current first, then compute power: P = VI or P = I²R

2. Thévenin's Theorem

2.1 Principle

ParameterDefinition
StatementAny linear two-terminal network can be replaced by an equivalent circuit consisting of a voltage source VTH in series with a resistance RTH
VTHOpen-circuit voltage across the terminals when load is removed
RTHEquivalent resistance looking into the terminals with all independent sources deactivated

2.2 Determining VTH

  • Remove the load from the terminals
  • Calculate the open-circuit voltage VOC across the terminals
  • VTH = VOC

2.3 Determining RTH

2.3.1 Method 1: Direct Calculation

  • Remove the load
  • Deactivate all independent sources (short voltage sources, open current sources)
  • Calculate resistance looking back into the circuit from the terminals
  • Dependent sources remain active but do not contribute without excitation

2.3.2 Method 2: Short-Circuit Current

  • Calculate short-circuit current ISC when terminals are shorted
  • RTH = VTH / ISC = VOC / ISC
  • Use when circuit contains dependent sources

2.3.3 Method 3: Test Source

  • Apply a test voltage VT or test current IT at the terminals
  • Calculate resulting current IT or voltage VT
  • RTH = VT / IT
  • Deactivate all independent sources; keep dependent sources active

2.4 Applications

  • Simplifies analysis when varying a single load element
  • Maximum power transfer analysis
  • Circuit design and troubleshooting

3. Norton's Theorem

3.1 Principle

ParameterDefinition
StatementAny linear two-terminal network can be replaced by an equivalent circuit consisting of a current source IN in parallel with a resistance RN
INShort-circuit current through the terminals when load is replaced by a short circuit
RNEquivalent resistance looking into the terminals with all independent sources deactivated; RN = RTH

3.2 Determining IN

  • Short-circuit the terminals where load was connected
  • Calculate the short-circuit current ISC flowing through the short
  • IN = ISC

3.3 Determining RN

  • Same methods as RTH (RN = RTH)
  • Alternatively: RN = VOC / ISC

3.4 Thévenin-Norton Conversion

ConversionRelationships
Thévenin to NortonIN = VTH / RTH; RN = RTH
Norton to ThéveninVTH = IN × RN; RTH = RN

4. Maximum Power Transfer Theorem

4.1 DC Circuits

ConceptDescription
ConditionMaximum power is transferred to the load when load resistance RL = RTH
Maximum PowerPmax = VTH² / (4RTH)
Efficiencyη = 50% at maximum power transfer (half dissipated in source resistance)
Load VoltageVL = VTH / 2 when RL = RTH
Load CurrentIL = VTH / (2RTH) when RL = RTH

4.2 AC Circuits

Load TypeCondition for Maximum Power
Resistive LoadRL = |ZTH| (magnitude of Thévenin impedance)
Complex LoadZL = ZTH* (complex conjugate of Thévenin impedance)
Maximum Power (Complex)Pmax = |VTH|² / (4RTH) where RTH = Re{ZTH}

4.3 Key Points

  • If ZTH = RTH + jXTH, then ZL = RTH - jXTH for maximum power
  • Reactive components in load cancel reactive components in source
  • Practical systems operate at higher efficiency, not maximum power transfer

5. Source Transformation

5.1 Principle

TransformationDescription
Voltage to CurrentVoltage source VS in series with R → Current source IS = VS/R in parallel with R
Current to VoltageCurrent source IS in parallel with R → Voltage source VS = IS × R in series with R
ResistanceResistance value R remains the same in both representations

5.2 Applications

  • Simplify circuits by converting between source types
  • Combine parallel current sources or series voltage sources
  • Cannot transform ideal sources (R = 0 for ideal voltage source, R = ∞ for ideal current source)
  • Polarity: positive terminal of VS corresponds to direction of IS leaving the source

6. Millman's Theorem

6.1 Principle

ConceptDescription
StatementFor parallel branches with voltage sources and series resistances, the common voltage across all branches can be calculated directly
FormulaV = (V₁/R₁ + V₂/R₂ + ... + Vn/Rn) / (1/R₁ + 1/R₂ + ... + 1/Rn)
Alternative FormV = (V₁G₁ + V₂G₂ + ... + VnGn) / (G₁ + G₂ + ... + Gn) where G = 1/R

6.2 Procedure

  • Identify all parallel branches with voltage sources and series resistances
  • Convert each branch to equivalent conductance G = 1/R
  • Apply formula to find common node voltage
  • Calculate branch currents using Ohm's law

7. Substitution Theorem

7.1 Principle

ConceptDescription
StatementAny branch in a network with voltage V and current I can be replaced by a voltage source of value V or a current source of value I without affecting the rest of the circuit
Voltage Source ReplacementReplace branch with voltage source equal to the voltage across the branch (maintain polarity)
Current Source ReplacementReplace branch with current source equal to the current through the branch (maintain direction)

7.2 Applications

  • Simplify analysis by replacing complex branches
  • Isolate portions of circuits for separate analysis
  • Must know voltage and current in branch before substitution

8. Reciprocity Theorem

8.1 Principle

ConceptDescription
StatementIn a linear bilateral network, if a voltage source V in branch A produces current I in branch B, then the same voltage source V in branch B will produce the same current I in branch A
Bilateral NetworkCircuit elements have the same characteristics regardless of current direction (resistors, inductors, capacitors)
LimitationDoes not apply to networks with dependent sources or nonlinear elements

8.2 Applications

  • Verify circuit calculations by interchanging source and response locations
  • Simplify measurements in testing (swap excitation and measurement points)
  • Antenna theory: transmitting and receiving patterns are identical

9. Compensation Theorem

9.1 Principle

ConceptDescription
StatementIf impedance Z in a branch changes by ΔZ, the change in current throughout the network can be calculated by inserting a voltage source V = -I × ΔZ in series with the changed branch
Change in CurrentΔI = change in current due to impedance change ΔZ
Compensation VoltageVcomp = -Ioriginal × ΔZ (opposes original current direction)

9.2 Applications

  • Analyze effects of component tolerance variations
  • Determine sensitivity of circuits to parameter changes
  • Calculate changes without re-analyzing entire circuit

10. Tellegen's Theorem

10.1 Principle

ConceptDescription
StatementFor any lumped network satisfying Kirchhoff's laws, the sum of instantaneous powers in all branches equals zero: Σ(vk × ik) = 0
InterpretationTotal power delivered equals total power absorbed in any network
ApplicabilityApplies to linear and nonlinear networks, time-varying or time-invariant

10.2 Key Points

  • Based solely on topology (KCL and KVL), not element characteristics
  • Valid for AC and DC circuits
  • Used in power conservation verification and network analysis validation

11. Application Guidelines

11.1 Theorem Selection

Use CaseRecommended Theorem
Multiple sources, finding one responseSuperposition
Varying single load, multiple calculationsThévenin or Norton
Maximum power to loadMaximum Power Transfer
Parallel voltage sourcesMillman's Theorem
Mixing series and parallel sourcesSource Transformation

11.2 Common Mistakes

  • Applying superposition to power calculations (must use voltage/current first)
  • Forgetting to keep dependent sources active during Thévenin/Norton calculation
  • Incorrect source deactivation (voltage source → short, current source → open)
  • Confusing maximum power transfer with maximum efficiency
  • Attempting to transform ideal sources without series/parallel resistance
The document Cheatsheet: Network Theorems is a part of the PE Exam Course Electrical & Computer Engineering for PE.
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