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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
Semiconductors and Semiconductor Devices

Concepts Of Physics MCQ Edition [Volume 2] · Physics · Semiconductors and Semiconductor Devices

Determine the current through the resistance R in the figure if R =...

Determine the current through the resistance RR in the figure if R=12ΩR = 12\Omega.
Determine the current through the resistance R in the figure if R = 12 .

Options

  1. A0.50 A0.50\text{ A}
  2. B0.83 A0.83\text{ A}
  3. C0.49 A0.49\text{ A}
  4. D0.42 A0.42\text{ A}

Correct answer

D. 0.42 A0.42\text{ A}

Step-by-step solution

Let the right common junction of the circuit be the reference node with a potential of 0 V0\text{ V}, and let the left common junction have a potential VV.

From the given circuit diagram, we can identify the polarities of the batteries:
- In the top branch, the longer line of the battery symbol is on the left, indicating the positive terminal is connected to the left node. Thus, the potential after the battery (moving right) is V−4V - 4.
- In the middle branch, the shorter, thicker line is on the left, indicating the negative terminal is connected to the left node. Thus, the potential after the battery is V−(−6)=V+6V - (-6) = V + 6.
- The diode in the bottom branch has its p-side (triangle) on the left and n-side (line) on the right, meaning it only conducts if V>0V > 0.

Let us initially assume the diode is reverse-biased (OFF), so no current flows through the bottom branch.
Applying Kirchhoff's Current Law (KCL) at the left node for the top and middle branches:
V−412+V−(−6)12=0\dfrac{V - 4}{12} + \dfrac{V - (-6)}{12} = 0

V−4+V+612=0\dfrac{V - 4 + V + 6}{12} = 0

2V+2=0⇒V=−1 V2V + 2 = 0 \Rightarrow V = -1\text{ V}

Now, we verify the state of the diode. The potential difference across the diode branch is V−0=−1 VV - 0 = -1\text{ V}. Since the potential at the p-side is lower than the n-side (−1 V<0 V-1\text{ V} < 0\text{ V}), the diode is indeed reverse-biased. Our assumption is correct, and the bottom branch acts as an open circuit.

The current through the resistance R=12ΩR = 12\Omega in the middle branch is:
IR=V−(−6)12=−1+612=512 AI_R = \dfrac{V - (-6)}{12} = \dfrac{-1 + 6}{12} = \dfrac{5}{12}\text{ A}

IR≈0.4167 AI_R \approx 0.4167\text{ A}

Rounding to two decimal places, we get 0.42 A0.42\text{ A}.

Answer: 0.42 A0.42\text{ A}
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