A brief note on Cells, the Meter Bridge and the Potentiometer . Read it before a test. Try each question at the end before you open its answer.
Cells in combination Series, aiding: E = E 1 + E 2 E = E_1 + E_2 E = E 1 + E 2 . Opposing: E = E 1 − E 2 E = E_1 - E_2 E = E 1 − E 2 . Always r = r 1 + r 2 r = r_1 + r_2 r = r 1 + r 2 . Charging cell: V = E + I r V = E + Ir V = E + I r . Discharging cell: V = E − I r V = E - Ir V = E − I r . Two cells in parallel: E = E 1 r 2 + E 2 r 1 r 1 + r 2 E = \dfrac{E_1r_2 + E_2r_1}{r_1 + r_2} E = r 1 + r 2 E 1 r 2 + E 2 r 1 and r = r 1 r 2 r 1 + r 2 r = \dfrac{r_1r_2}{r_1 + r_2} r = r 1 + r 2 r 1 r 2 . m m m rows of k k k cells: E = k E 0 E = kE_0 E = k E 0 and r = k r 0 m r = \dfrac{kr_0}{m} r = m k r 0 . Greatest current: R = k r 0 m R = \dfrac{kr_0}{m} R = m k r 0 , so m = N r 0 R m = \sqrt{\dfrac{Nr_0}{R}} m = R N r 0 . The meter bridge Balance: X R = l 100 − l \dfrac{X}{R} = \dfrac{l}{100 - l} R X = 100 − l l , with l l l measured from the side of X X X . Does not depend on: the emf of the cell or the galvanometer. Best accuracy: a balance point near 50 cm 50\ \text{cm} 50 cm . The fractional error is 100 δ l l ( 100 − l ) \dfrac{100\,\delta l}{l(100 - l)} l ( 100 − l ) 100 δ l . Interchange: the balance point becomes about 100 − l 100 - l 100 − l . Average the two values of X X X to reduce the end corrections. Resistivity: ρ = π d 2 X 4 L \rho = \dfrac{\pi d^2 X}{4L} ρ = 4 L π d 2 X . The potentiometer Gradient: k = I R w L k = \dfrac{IR_w}{L} k = L I R w . Potential: V = k l V = kl V = k l . Balance: E = k l E = kl E = k l , so E 1 E 2 = l 1 l 2 \dfrac{E_1}{E_2} = \dfrac{l_1}{l_2} E 2 E 1 = l 2 l 1 . Internal resistance: r = R l 1 − l 2 l 2 r = R\,\dfrac{l_1 - l_2}{l_2} r = R l 2 l 1 − l 2 , with l 1 l_1 l 1 for the open cell. True emf: at balance no current is drawn, so nothing is lost inside the cell. More sensitive: a smaller gradient, with the balance still on the wire. The driver emf must be larger than the emf measured. A worked example A cell balances at 300 cm 300\ \text{cm} 300 cm when open, and at 250 cm 250\ \text{cm} 250 cm with a 5.0 Ω 5.0\ \Omega 5.0 Ω resistor across it. Find its internal resistance.
The rule. r = R l 1 − l 2 l 2 r = R\,\dfrac{l_1 - l_2}{l_2} r = R l 2 l 1 − l 2 . The numbers. r = 5.0 Ω × 300 − 250 250 = 1.0 Ω r = 5.0\ \Omega \times \dfrac{300 - 250}{250} = 1.0\ \Omega r = 5.0 Ω × 250 300 − 250 = 1.0 Ω . Practice with new numbers
A program to try The program finds the emf, resistance and current of a group of 20 20 20 cells in 5 5 5 rows.
Run it. Compare each line with the rules above.
1. Change m, k = 5, 4 to m, k = 4, 5. Does the current rise or fall?
Mistakes to avoid Subtracting resistances for opposing cells. Only the emfs subtract. Using k r kr k r for a group. The rows are in parallel, so it is k r / m kr/m k r / m . Turning the bridge ratio upside down. The length on the side of X X X goes on top. Putting l 1 l_1 l 1 on the bottom in the internal resistance formula. The closed length l 2 l_2 l 2 goes there. Check yourself What is the emf of two cells of 5.0 V 5.0\ \text{V} 5.0 V and 3.0 V 3.0\ \text{V} 3.0 V joined in series, opposing? Stuck? Show a hint Show the answerA meter bridge has a 20 Ω 20\ \Omega 20 Ω box in the right gap and balances at 25 cm 25\ \text{cm} 25 cm . What is X X X ? Stuck? Show a hint Show the answerTwo cells balance at 200 cm 200\ \text{cm} 200 cm and 300 cm 300\ \text{cm} 300 cm . What is the ratio of their emfs? Stuck? Show a hint Show the answerWhy can a potentiometer not balance a cell of 3 V 3\ \text{V} 3 V if its driver cell is 2 V 2\ \text{V} 2 V ? Stuck? Show a hint Show the answer