Question
Question: Sliding contact of a potentiometer is in the middle of the potentiometer wire having resistance $R_p...
Sliding contact of a potentiometer is in the middle of the potentiometer wire having resistance Rp = 1Ω as shown in the figure. An external resistance of Re = 2Ω is connected via the sliding contact.
0.3 A
1.35 A
1.0 A
0.9 A
1.0 A
Solution
Solution Explanation: We model the circuit as follows:
- Let the potentiometer (total resistance 1 Ω) be split into two equal resistances: R₁ = 0.5 Ω (from battery positive to sliding contact) and R₂ = 0.5 Ω (from sliding contact to battery negative).
- Let V_A = 0.9 V (battery positive) and V_B = 0 V (battery negative).
- The external resistor Rₑ = 2 Ω is connected from the sliding contact (node C) to the negative terminal.
- Using Kirchhoff’s Current Law (KCL) at node C, where the currents coming from R₁ equal the currents leaving via R₂ and Rₑ, we write:
(V_A − V_C) / R₁ = V_C / R₂ + V_C / Rₑ
Substitute the known values:
(0.9 − V_C) / 0.5 = V_C / 0.5 + V_C / 2
Solve the equation step by step:
-
Multiply through by a common factor (say 2) to eliminate fractions: 2×[(0.9 − V_C) / 0.5] = 2×[V_C / 0.5] + 2×[V_C / 2] 4(0.9 − V_C) = 4V_C + V_C (since 2/0.5 = 4 and 2/2 = 1)
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Expand and solve: 3.6 − 4V_C = 5V_C 3.6 = 9V_C V_C = 0.4 V
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Now, the battery current is just the current flowing through R₁ (from the battery to node C): I₁ = (V_A − V_C) / R₁ = (0.9 − 0.4) / 0.5 = 0.5 / 0.5 = 1.0 A
Thus, the battery supplies a current of 1.0 A.