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Question: A uniform rod of length l is acted upon by a force F in a gravity-free region, as shown in the figur...

A uniform rod of length l is acted upon by a force F in a gravity-free region, as shown in the figure. If the area of cross-section of the rod is A and it's Young's modulus is Y, then the elastic potential energy stored in the rod due to elongation is U=F2lnAY. Then find the value of n?

Answer

6

Explanation

Solution

The problem describes a uniform rod of length ll acted upon by a force FF in a gravity-free region. The figure shows a single force FF applied at one end of the rod. In a gravity-free region, if a single force FF is applied to a free body of mass mm, the body accelerates with a=F/ma = F/m. In this case, the tension within the rod is not uniform; it varies along the length.

Let's assume the force FF is applied at one end, say the end at x=lx=l, and the other end is at x=0x=0. Let the rod have mass mm. The acceleration of the rod is a=F/ma = F/m. Consider a cross-section at a distance xx from the free end (at x=0x=0, where no force is applied). The part of the rod from 00 to xx has mass m(x/l)m(x/l). This part is accelerated by the tension T(x)T(x) at the cross-section at xx.

Using Newton's second law for the segment from 00 to xx: T(x)=(mass of segment)×(acceleration)T(x) = (\text{mass of segment}) \times (\text{acceleration}) T(x)=(mlx)a=(mlx)(Fm)=FxlT(x) = \left(\frac{m}{l} x\right) a = \left(\frac{m}{l} x\right) \left(\frac{F}{m}\right) = \frac{Fx}{l}. The tension varies linearly from 00 at the free end (x=0x=0) to FF at the end where the force is applied (x=lx=l).

The strain at a distance xx from the free end is given by Hooke's law: ϵ(x)=Stress(x)Y=T(x)/AY=Fx/lAY=FxlAY\epsilon(x) = \frac{\text{Stress}(x)}{Y} = \frac{T(x)/A}{Y} = \frac{Fx/l}{AY} = \frac{Fx}{lAY}.

The elastic potential energy stored in a small element of length dxdx at position xx is given by: dU=12×Stress(x)×Strain(x)×Volume of elementdU = \frac{1}{2} \times \text{Stress}(x) \times \text{Strain}(x) \times \text{Volume of element} dU=12×T(x)A×ϵ(x)×(Adx)dU = \frac{1}{2} \times \frac{T(x)}{A} \times \epsilon(x) \times (A dx) dU=12T(x)ϵ(x)dxdU = \frac{1}{2} T(x) \epsilon(x) dx Substitute the expressions for T(x)T(x) and ϵ(x)\epsilon(x): dU=12(Fxl)(FxlAY)dx=12F2x2l2AYdxdU = \frac{1}{2} \left(\frac{Fx}{l}\right) \left(\frac{Fx}{lAY}\right) dx = \frac{1}{2} \frac{F^2 x^2}{l^2 AY} dx.

To find the total elastic potential energy stored in the rod, integrate dUdU over the entire length of the rod from x=0x=0 to x=lx=l: U=0ldU=0lF2x22l2AYdxU = \int_0^l dU = \int_0^l \frac{F^2 x^2}{2 l^2 AY} dx. Since FF, ll, AA, and YY are constants with respect to the integration variable xx: U=F22l2AY0lx2dxU = \frac{F^2}{2 l^2 AY} \int_0^l x^2 dx. Evaluate the integral: 0lx2dx=[x33]0l=l33033=l33\int_0^l x^2 dx = \left[\frac{x^3}{3}\right]_0^l = \frac{l^3}{3} - \frac{0^3}{3} = \frac{l^3}{3}.

Substitute the result of the integral back into the expression for UU: U=F22l2AY(l33)=F2l36l2AY=F2l6AYU = \frac{F^2}{2 l^2 AY} \left(\frac{l^3}{3}\right) = \frac{F^2 l^3}{6 l^2 AY} = \frac{F^2 l}{6AY}.

The elastic potential energy stored in the rod is U=F2l6AYU = \frac{F^2 l}{6AY}. The question gives the formula for the elastic potential energy stored in the rod as U=F2lnAYU = \frac{F^2 l}{nAY}. Comparing the calculated formula with the given formula: F2l6AY=F2lnAY\frac{F^2 l}{6AY} = \frac{F^2 l}{nAY}. By comparing the denominators, we can see that n=6n=6.

The final answer is 6\boxed{6}.

Explanation of the solution:

  1. Determine the tension distribution along the rod when a force F is applied at one end in a gravity-free region. The tension varies linearly from 0 at the free end to F at the end where the force is applied. T(x)=Fx/lT(x) = Fx/l, where x is the distance from the free end.
  2. Calculate the strain at each point along the rod using Hooke's Law: ϵ(x)=T(x)/(AY)=Fx/(lAY)\epsilon(x) = T(x)/(AY) = Fx/(lAY).
  3. Calculate the elastic potential energy stored in an infinitesimal element of length dxdx at position xx: dU=12T(x)ϵ(x)dx=12F2x2l2AYdxdU = \frac{1}{2} T(x) \epsilon(x) dx = \frac{1}{2} \frac{F^2 x^2}{l^2 AY} dx.
  4. Integrate the potential energy density over the length of the rod to find the total potential energy: U=0ldU=0lF2x22l2AYdx=F22l2AY0lx2dx=F22l2AYl33=F2l6AYU = \int_0^l dU = \int_0^l \frac{F^2 x^2}{2 l^2 AY} dx = \frac{F^2}{2 l^2 AY} \int_0^l x^2 dx = \frac{F^2}{2 l^2 AY} \frac{l^3}{3} = \frac{F^2 l}{6AY}.
  5. Compare the calculated potential energy formula U=F2l6AYU = \frac{F^2 l}{6AY} with the given formula U=F2lnAYU = \frac{F^2 l}{nAY} to find the value of nn. The comparison yields n=6n=6.