6 Cell, Emf, Internal Resistance Cells in Series and Parallel
Cell, Emf, Internal Resistance Cells in Series and Parallel
Emf
- Potential difference between the two poles of the cell in an open circuit is called emf of the cell.
SI unit is volt (V).
Internal resistance (r) of cell
- Resistance offered by the electrolyte of the cell when the electric current flows through it
E − emf of cell
r − Internal resistance of the cell
R − External resistance
K − Key
V − Voltmeter
- The key K is closed and a current I flows in the circuit.
According to Ohm’s law,
- Let V be the terminal potential difference. The terminal potential difference V is less than emf E of the cell by an equal amount, which is equal to potential drop across external resistance R i.e.,
∴ V = E − Ir
Also, terminal potential difference is equal to potential differences across external resistance.
VÂ =Â IR
From equation (1),
Combination of cells
Cells in Series
E1 E2 − emf of two cells
r1, r2 − Internal resistance of two cells
I − Current in the circuit
Terminal potential difference across the first cell, V1 = E1 − Ir1
Terminal potential difference across the second cell, V2 = E2 − Ir2
Potential difference between the points A and B,
V = V1 + V2 = (E1 − Ir1) + (E2 − Ir2)
= (E1 + E2) − I (r1 + r2)
Let
E − Effective emf
r − Effective internal resistance
V = E − Ir
∴ E = E1 + E2
r = r1 + r2
- Current in the circuit,
- If the two cells are connected in opposite direction, then
E = E1 − E2
Cell in Parallel
E1, E2 − emf of two cells
r1, r2 − Internal resistances of cell
I1, I2 − Current due to the two cells
Terminal potential difference across the first cell,
V = E1 − I1r1
For the second cell,
Let E be effective emf and r is effective internal resistance.
V = E − Ir
And,
Mixed Grouping of Cells
Suppose ‘n’ cells of emf ‘E’ and internal resistance ‘r’ are connected in series in each branch; and there are ‘m’ such branches. ‘R’ is the external resistance connected to the circuit.
In each branch, the net emf is nE and the net internal resistance is nr. The equivalent resistance of all the internal resistances in parallel is,
We finally have a circuit with a cell of emf nE, internal resistance connected to a resistance R. The current through the circuit is,