Step 1: Understanding the Concept:
For a rod to remain horizontal in equilibrium, the net torque about the point of suspension \(P\) must be zero.
Torque is the product of the force and its perpendicular distance from the pivot.
The weights acting are the suspended mass \(m\) at end \(A\) and the weight of the uniform rod (\(M\)) acting at its center of mass.
Step 2: Key Formula or Approach:
Torque balance: \(\sum \tau_P = 0\).
Weight of rod acts at center \(L/2\).
Step 3: Detailed Explanation:
Let \(L\) be the total length of the uniform rod and \(M\) be its mass.
Pivot is at point \(P\), at distance \(x\) from end \(A\).
Distance from \(A\) to \(P = x\).
Distance from \(P\) to the center of mass (midpoint) of the rod \(= (L/2) - x\).
Taking torques about \(P\):
Anti-clockwise torque due to \(m\): \(\tau_1 = (mg) \cdot x\).
Clockwise torque due to rod's weight \(M\): \(\tau_2 = (Mg) \cdot (L/2 - x)\).
Equating torques:
\[mx = M(L/2 - x)\]
\[mx = \frac{ML}{2} - Mx\]
\[x(m + M) = \frac{ML}{2}\]
We want to see the relationship between \(m\) and \(x\).
\[m + M = \frac{ML}{2} \cdot \frac{1}{x}\]
\[m = \left(\frac{ML}{2}\right) \frac{1}{x} - M\]
This is of the form \(y = k \cdot Z + C\), where \(y = m\) and \(Z = 1/x\).
Thus, a plot of \(m\) versus \(1/x\) will yield a straight line with a negative intercept.
This matches option (C).
Step 4: Final Answer:
From the torque balance equation, \(m\) is linearly proportional to the reciprocal of the distance \(x\). Thus, plotting \(m\) against \(1/x\) gives a straight line.