Step 1: Understand the circuit.
Two resistors of \(50k\Omega\) each are in series across a \(100V\) source.
Point \(B\) is between the two resistors, and voltmeter is connected across \(B\) and \(C\), i.e. across the lower \(50k\Omega\) resistor.
Step 2: Equivalent resistance of lower branch.
Voltmeter resistance \(R_v\) is in parallel with lower \(50k\Omega\):
\[
R_{eq} = \frac{50k \cdot R_v}{50k + R_v}
\]
Step 3: Total series resistance.
Upper resistor is \(50k\Omega\), so total:
\[
R_{total} = 50k + R_{eq}
\]
Step 4: Use voltage division.
Voltmeter reads potential across lower part:
\[
V_{BC} = \frac{R_{eq}}{50k + R_{eq}}\cdot 100
\]
Given:
\[
V_{BC} = \frac{100}{3}
\]
So:
\[
\frac{100}{3} = \frac{R_{eq}}{50k + R_{eq}}\cdot 100
\Rightarrow \frac{1}{3} = \frac{R_{eq}}{50k + R_{eq}}
\]
Step 5: Solve for \(R_{eq}\).
\[
50k + R_{eq} = 3R_{eq}
\Rightarrow 50k = 2R_{eq}
\Rightarrow R_{eq} = 25k\Omega
\]
Step 6: Solve for \(R_v\).
\[
25k = \frac{50k \cdot R_v}{50k + R_v}
\]
Cross multiply:
\[
25k(50k + R_v) = 50kR_v
\]
\[
1250k^2 + 25kR_v = 50kR_v
\]
\[
1250k^2 = 25kR_v
\Rightarrow R_v = 50k\Omega
\]
Final Answer:
\[
\boxed{50\,k\Omega}
\]