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Thevenin's Theorem Equivalent Resistance

This is the resistance you would see looking into two terminals if you switched off every independent source (short out voltage sources and open up current sources). You can also find it by dividing the open-circuit voltage by the short-circuit current. It matters because it sets how much a source sags when you draw current from it, and it is used to work out maximum power transfer.

Circuit Analysis Network Theorem

Thevenin Equivalent Resistance Calculator

Any linear circuit seen from two terminals behaves like a voltage source VOC in series with a resistance RTH. Divide the open-circuit voltage by the short-circuit current to get RTH. Enter any two of RTH, VOC and ISC and the third is solved. Then see the Norton equivalent and the power delivered to a load.

RTH = VOC / ISCPmax = VOC² / (4RTH)
Solve for
Load resistance RL (for power and efficiency)
Ω
Above 0.
—
Load power ÷ maximum power
0%25%50%75%100%
—

Step-by-step solution

Norton equivalent and load results

Find VOC, ISC and RTH from a circuit

A. Voltage divider source (Vs with R1 in series and R2 across the output)
Source Vs
V
R1 (series)
Ω
R2 (shunt)
Ω
B. Two load measurements on the same source
Load Ra
Ω
Voltage Va across Ra
V
Load Rb
Ω
Voltage Vb across Rb
V

A: VOC = VsR2/(R1+R2), RTH = R1 ∥ R2. B: RTH = (Vb − Va) / (Va/Ra − Vb/Rb), then VOC = Va(1 + RTH/Ra).

Thevenin and Norton equivalents

The two circuits give identical voltage and current at the terminals for any load.

Load power and efficiency versus RL

Reference data

Your source feeding loads of different size
RLVLILPLEfficiency
Typical source resistances (approximate)
SourceTypical RTHNote
Car battery (12 V lead-acid)5 to 20 mΩVery stiff, delivers hundreds of amps
Fresh AA alkaline cell0.1 to 0.3 ΩRises as the cell discharges
9 V alkaline battery1 to 3 ΩPoor at high current
Function generator output50 ΩMatched to 50 Ω cable
Bench power supply (regulated)under 10 mΩWithin the current limit
Piezo or high-impedance sensorkΩ to MΩNeeds a high-impedance input

Values vary with temperature, state of charge and model. Your row is highlighted when the load equals RTH (maximum power point).

FAQ

What is Thevenin's theorem?

Any linear circuit with two output terminals can be replaced by a single voltage source VTH in series with a resistor RTH. VTH is the open-circuit terminal voltage and RTH is the resistance seen at the terminals with independent sources turned off.

Why is RTH = VOC / ISC?

Shorting the terminals makes the whole open-circuit voltage drop across RTH, so ISC = VOC/RTH. Rearranged, RTH = VOC/ISC. This is a convenient measurement or calculation shortcut.

What is maximum power transfer?

A load takes the most power when RL = RTH. Then Pmax = VOC²/(4RTH), but the efficiency is only 50% because half the power is lost in the source resistance.

Is it safe to short-circuit a real source to measure ISC?

Often not. Batteries and supplies can overheat or fail. It is safer to measure the voltage across two known loads (method B above) and compute RTH from them.

Educational tool only. The Thevenin model applies to linear circuits with constant sources and resistances. Real batteries and non-linear devices change with load and temperature. Never short-circuit a real power source unless it is rated for it.

Variables

Symbol Quantity Unit
R_TH Thevenin equivalent resistance Ω
V_OC Open-circuit voltage V
I_SC Short-circuit current A

What it means

Thévenin’s theorem simplifies any linear circuit to a single voltage source (V_TH) in series with a single resistance (R_TH). The Thévenin voltage V_TH is the open‑circuit voltage at the terminals. The Thévenin resistance R_TH is the equivalent resistance seen from the terminals with all independent sources turned off (voltage sources shorted, current sources opened). R_TH can also be found as the ratio V_TH / I_SC, where I_SC is the short‑circuit current. This theorem is invaluable for analyzing circuits with multiple sources and varying loads. It reduces a complex network to a simple series circuit, making it easy to determine the load current and voltage. The theorem is widely used in power systems, amplifier design, and signal processing. Example: If the open‑circuit voltage across the terminals is 10V and the short‑circuit current is 2A, then R_TH = 10V / 2A = 5Ω. The Thévenin equivalent is a 10V source in series with 5Ω.

Worked example

Thevenin's Theorem – Practical Example

Real‑World
Scenario: For the same circuit, you measure the open‑circuit voltage (VOC = 10 V) and short‑circuit current (ISC = 2 A). Find the Thevenin resistance RTH.
ParameterValue
VOC10 V
ISC2 A
FormulaRTH = VOC / ISC
1Apply formula:RTH = 10 V / 2 A
2Calculate:RTH = 5 Ω
Final Design RTH = 5 Ω ✓ Equivalent resistance
Why: RTH is found by dividing VOC by ISC – this gives the effective internal resistance.

Common mistakes

  • V_OC: Open‑circuit voltage across the terminals – not the voltage across a load.
  • I_SC: Short‑circuit current – the current that flows when the terminals are shorted.
  • R_TH: The ratio V_OC / I_SC – also the equivalent resistance with sources deactivated.
  • Dependent sources: For R_TH, you cannot simply deactivate dependent sources – use a test source or compute V_OC/I_SC.
  • Maximum power: R_TH is the load resistance that maximises power transfer (when R_L = R_TH).

Applications

Thévenin's theorem reduces any linear circuit to a single voltage source (V_TH) in series with a single resistance (R_TH). V_TH is the open‑circuit voltage, and R_TH is the resistance seen from the terminals. This theorem is a cornerstone of circuit analysis, enabling engineers to simplify networks for design and troubleshooting. It is used to analyse power supplies, to determine load voltage and current, and to design matching networks. By applying Thévenin's theorem, professionals can quickly assess the effect of changing loads without re‑analysing the entire circuit. It is also used in the calculation of maximum power transfer and in the design of operational amplifier circuits. Mastering Thévenin's theorem is essential for any electrical engineer.

  • Network simplification for load analysis
  • Design of voltage sources and regulators
  • Maximum power transfer and impedance matching
  • Fault analysis and circuit protection design
  • Educational cornerstone of circuit theory