
To solve the problem, we first need to understand the circuit configuration and apply the concept of equivalent resistance.
The circuit consists of a series-parallel combination of resistors as shown in the figure above.
Given:
Step 1: Analyze the Circuit Configuration
The resistors \( 2R \Omega \) and \( X \Omega \) are in parallel. The equivalent resistance \( R_{eq1} \) of these two resistors is given by:
R_{eq1} = \frac{(2R \cdot X)}{(2R + X)}Step 2: Find the Total Equivalent Resistance
The equivalent resistance \( R_{eq1} \) is in series with \( R \Omega \). Therefore, the total equivalent resistance \( R_{total} \) is:
R_{total} = R + R_{eq1} = R + \frac{(2R \cdot X)}{(2R + X)}We know from the problem statement that the total equivalent resistance between \( A \) and \( B \) is \( X \Omega \). Therefore, we equate:
X = R + \frac{(2R \cdot X)}{(2R + X)}Step 3: Solve for \( X \)
Multiply through by \( (2R + X) \) to eliminate the fraction:
X(2R + X) = R(2R + X) + 2RXThe equation simplifies to:
2RX + X^2 = 2R^2 + RX + 2RXBy cancelling \( 2RX \) from both sides, we get:
X^2 - RX - 2R^2 = 0This is a quadratic equation in terms of \( X \). Solving for \( X \) using the quadratic formula:
X = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}Here, \( a = 1 \), \( b = -R \), and \( c = -2R^2 \).
X = \frac{R \pm \sqrt{R^2 + 8R^2}}{2} = \frac{R \pm \sqrt{9R^2}}{2} = \frac{R \pm 3R}{2}This gives two solutions:
Since resistance cannot be negative, we have:
Option 2 \((\sqrt{3} - 1)R\) is the correct choice based on the given options.
Therefore, the value of \( X \) is \((\sqrt{3} - 1)R\).
A thin uniform rod (\(X\)) of mass \(M\) and length \(L\) is pivoted at a height \( \left(\dfrac{L}{3}\right) \) as shown in the figure. The rod is allowed to fall from a vertical position and lie horizontally on the table. The angular velocity of this rod when it hits the table top is ________. (\(g\) = gravitational acceleration) 