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QPages 12-14: Q32: HC Verma: Concepts of Physics - Volume 2 Heat and Temperature Pages 12-14: Q32 Solution: Show that the moment of inertia of a solid body of any shape…

⚠️ Common Exam Traps & Conceptual Pitfalls

Students frequently replace the radius $r$ with $r(1+\alpha\theta)$ and then write $I=I_0(1+\alpha\theta)$, forgetting that $I$ involves $r^2$; the correct substitution gives $r^2\to r^2(1+\alpha\theta)^2\approx r^2(1+2\alpha\theta)$ for small temperature changes. Remember to square the linear expansion factor and use the first‑order approximation only after expanding.

Show that the moment of inertia of a solid body of any shape changes with temperature as I=I01+2αθ)I = I_0 1 + 2\alpha\theta), where I0I_0 is the moment of inertia at 0�C and α\alpha is the coefficient of linear expansion of the solid.

Step-by-Step Verified Solution

**Answer:** I=I0(1+2αθ)I = I_0(1 + 2\alpha\theta) **Step-by-Step Explanation:** For a solid body, moment of inertia I=∫r2dmI = \int r^2 dm. When heated, all linear dimensions scale as r→r(1+αθ)r \to r(1 + \alpha\theta). So r2→r2(1+αθ)2≈r2(1+2αθ)r^2 \to r^2(1 + \alpha\theta)^2 \approx r^2(1 + 2\alpha\theta). Mass dmdm is unchanged (mass conservation). Hence I=I0(1+2αθ)I = I_0(1 + 2\alpha\theta).

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