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Formulas/physics/Current Electricity/Potentiometer — Internal Resistance

Potentiometer — Internal Resistance

Internal resistance of a cell measured using a potentiometer. l₁ is balance length with cell in open circuit, l₂ with external resistance R connected. Derived from EMF and terminal voltage comparison.
Class 11Class 12
Derivation

Setup

Cell under test (EMF E\mathcal{E}, internal resistance rr) connected to the potentiometer.

Step 1: Switch SS open (cell in open circuit). Balance length =l1= l_1. Since no current flows:

E=ϕl1\mathcal{E} = \phi l_1

Step 2: Switch SS closed — external resistance RR connected across the cell. Balance length =l2= l_2. Current I=E/(R+r)I = \mathcal{E}/(R+r) flows; terminal voltage:

V=EIr=IR=ϕl2V = \mathcal{E} - Ir = IR = \phi l_2

Derivation

Dividing the two equations:

EV=l1l2    EIR=l1l2\frac{\mathcal{E}}{V} = \frac{l_1}{l_2} \implies \frac{\mathcal{E}}{IR} = \frac{l_1}{l_2}

Also E=I(R+r)\mathcal{E} = I(R + r), so E/IR=(R+r)/R\mathcal{E}/IR = (R+r)/R:

R+rR=l1l2    r=R(l1l21)\frac{R + r}{R} = \frac{l_1}{l_2} \implies r = R\left(\frac{l_1}{l_2} - 1\right) r=R(l1l2l2)\boxed{r = R\left(\frac{l_1 - l_2}{l_2}\right)}
Note
$l_1 > l_2$ always — the terminal voltage under load is less than the open-circuit EMF. If $l_1 = l_2$, the internal resistance is zero (ideal cell).