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Q.a. Derive an expression for elastic potential energy of a strained body. OR b. Show that the relation between the three coefficients of thermal expansion is given by γ=3β2=3α\gamma = \dfrac{3\beta}{2} = 3\alpha.

Nagaland NbseNagaland Board of School Education (Class XI) 2025Subjective· 3mImportance★★★★★
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When a body is elastically strained (e.g. a wire stretched within its elastic limit), the work done by the external force is stored as elastic potential energy; this is found by integrating the work done against the internal restoring force as the strain builds up from zero.

Consider a wire of natural length LL and cross-sectional area AA, being stretched by an external force. Within the elastic limit, Young's modulus Y=stressstrain=F/AΔl/LY = \dfrac{\text{stress}}{\text{strain}} = \dfrac{F/A}{\Delta l/L}, so at an extension xx (where 0≤x≤ΔL0\le x\le \Delta L), the restoring (and hence applied) force is:

F(x)=YAxLF(x) = \dfrac{YAx}{L}

The work done in stretching the wire by a further small amount dxdx is dW=F(x) dxdW = F(x)\,dx. The total work done (= elastic PE stored) in stretching from x=0x=0 to x=ΔLx=\Delta L is:

U=∫0ΔLF(x) dx=∫0ΔLYAxL dx=YAL⋅(ΔL)22U = \int_0^{\Delta L} F(x)\,dx = \int_0^{\Delta L} \dfrac{YAx}{L}\,dx = \dfrac{YA}{L}\cdot\dfrac{(\Delta L)^2}{2}

U=12(YΔLL)(ΔLL)(AL)=12 (stress)(strain) (volume)U = \dfrac12 \left(\dfrac{Y\Delta L}{L}\right)\left(\dfrac{\Delta L}{L}\right)(AL) = \dfrac12\,(\text{stress})(\text{strain})\,(\text{volume})

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