Question:

In the given figure: \[ V_1=V,\quad V_2=\alpha V,\quad R_1=\beta R,\quad R_2=\gamma R, \] where \(\alpha,\beta,\gamma\) are positive real numbers. The value of current \(I\) is

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In bridge-type resistor circuits, first identify symmetry and then apply Kirchhoff's Voltage Law carefully. Express all resistances and voltages in terms of the given parameters before simplifying.
Updated On: Jun 25, 2026
  • \(\dfrac{(\alpha-1)\gamma}{4\beta(\beta+\gamma)}\dfrac{V}{R}\)
  • \(\dfrac{(\alpha-1)}{4\beta}\dfrac{V}{R}\)
  • \(\dfrac{(\alpha-1)\beta}{2\gamma(\beta+\gamma)}\dfrac{V}{R}\)
  • \(\dfrac{(\alpha-1)(\beta+\gamma)}{2\beta\gamma}\dfrac{V}{R}\)
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The Correct Option is A

Solution and Explanation

Step 1: Understand the symmetry of the circuit.
The circuit contains four equal resistors of value \[ R_1=\beta R \] and a central branch containing \[ R_2=\gamma R \] along with a source \(V_2=\alpha V\).
Using Kirchhoff's laws and symmetry, let the current in the right lower branch be \(I\).

Step 2: Apply Kirchhoff's Voltage Law.
The equivalent analysis of the bridge gives the current through the indicated branch as \[ I= \frac{V_2-V_1}{4R_1\left(1+\dfrac{R_1}{R_2}\right)} \] Substituting \[ V_1=V,\qquad V_2=\alpha V, \] we get \[ I= \frac{\alpha V-V}{4\beta R\left(1+\dfrac{\beta R}{\gamma R}\right)} \] \[ = \frac{(\alpha-1)V}{4\beta R\left(1+\dfrac{\beta}{\gamma}\right)} \]

Step 3: Simplify the denominator.
\[ 1+\frac{\beta}{\gamma} = \frac{\beta+\gamma}{\gamma} \] Hence, \[ I= \frac{(\alpha-1)V}{4\beta R\left(\dfrac{\beta+\gamma}{\gamma}\right)} \] \[ = \frac{(\alpha-1)\gamma}{4\beta(\beta+\gamma)} \cdot \frac{V}{R} \]

Step 4: Final conclusion.
Therefore, the current is \[ \boxed{ \dfrac{(\alpha-1)\gamma}{4\beta(\beta+\gamma)} \dfrac{V}{R} } \]
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