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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
Electric Current in Conductors

Concepts Of Physics MCQ Edition [Volume 2] · Physics · Electric Current in Conductors

A portion of an electric circuit is depicted in the figure. The...

A portion of an electric circuit is depicted in the figure. The electric potentials at points aa, bb, and cc are given as 30 V30 \text{ V}, 12 V12 \text{ V}, and 2 V2 \text{ V}, respectively. Determine the currents flowing through each of the three resistors.
A portion of an electric circuit is depicted in the figure. The electric potentials at points a , b , and c are given

Options

  1. A1 A1 \text{ A} through 10 Ω10 \text{ }\Omega, 0.6 A0.6 \text{ A} through 20 Ω20 \text{ }\Omega, and 0.4 A0.4 \text{ A} through 30 Ω30 \text{ }\Omega
  2. B2 A2 \text{ A} through 10 Ω10 \text{ }\Omega, 0.8 A0.8 \text{ A} through 20 Ω20 \text{ }\Omega, and 1.2 A1.2 \text{ A} through 30 Ω30 \text{ }\Omega
  3. C1 A1 \text{ A} through 10 Ω10 \text{ }\Omega, 0.4 A0.4 \text{ A} through 20 Ω20 \text{ }\Omega, and 0.6 A0.6 \text{ A} through 30 Ω30 \text{ }\Omega
  4. D0.5 A0.5 \text{ A} through 10 Ω10 \text{ }\Omega, 0.2 A0.2 \text{ A} through 20 Ω20 \text{ }\Omega, and 0.3 A0.3 \text{ A} through 30 Ω30 \text{ }\Omega

Correct answer

C. 1 A1 \text{ A} through 10 Ω10 \text{ }\Omega, 0.4 A0.4 \text{ A} through 20 Ω20 \text{ }\Omega, and 0.6 A0.6 \text{ A} through 30 Ω30 \text{ }\Omega

Step-by-step solution

Let the electric potential at the junction of the three resistors be VV.

Applying Kirchhoff's Current Law (KCL) at the junction, the sum of currents leaving the junction is zero. Assuming current flows from aa to the junction, and from the junction to bb and cc:

Va−V10=V−Vb20+V−Vc30\dfrac{V_a - V}{10} = \dfrac{V - V_b}{20} + \dfrac{V - V_c}{30}

Given that Va=30 VV_a = 30 \text{ V}, Vb=12 VV_b = 12 \text{ V}, and Vc=2 VV_c = 2 \text{ V}, we substitute these values into the equation:

30−V10=V−1220+V−230\dfrac{30 - V}{10} = \dfrac{V - 12}{20} + \dfrac{V - 2}{30}

Multiplying the entire equation by 6060 to clear the denominators:

6(30−V)=3(V−12)+2(V−2)6(30 - V) = 3(V - 12) + 2(V - 2)

180−6V=3V−36+2V−4180 - 6V = 3V - 36 + 2V - 4

180−6V=5V−40180 - 6V = 5V - 40

11V=220  ⟹  V=20 V11V = 220 \implies V = 20 \text{ V}

Now, we calculate the current through each resistor:

Current through the 10 Ω10 \text{ }\Omega resistor:
I10=Va−V10=30−2010=1 AI_{10} = \dfrac{V_a - V}{10} = \dfrac{30 - 20}{10} = 1 \text{ A}

Current through the 20 Ω20 \text{ }\Omega resistor:
I20=V−Vb20=20−1220=820=0.4 AI_{20} = \dfrac{V - V_b}{20} = \dfrac{20 - 12}{20} = \dfrac{8}{20} = 0.4 \text{ A}

Current through the 30 Ω30 \text{ }\Omega resistor:
I30=V−Vc30=20−230=1830=0.6 AI_{30} = \dfrac{V - V_c}{30} = \dfrac{20 - 2}{30} = \dfrac{18}{30} = 0.6 \text{ A}
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