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Question: A uniform dense rod with non uniform young's modulus is hanging from ceiling under gravity. If elast...

A uniform dense rod with non uniform young's modulus is hanging from ceiling under gravity. If elastic energy density at every point is same then young's modulus with x will change as which of the shown graph :-

A

A

B

B

C

C

D

D

Answer

C

Explanation

Solution

Let the rod have length ll, mass mm, and constant cross-sectional area AA. Let xx be the distance measured from the top end of the rod (hanging from the ceiling), so x=0x=0 at the top and x=lx=l at the bottom. The rod has a uniform density ρ\rho.

The tension T(x)T(x) at a point xx is the weight of the rod below that point. The mass of the segment from xx to ll is dm=ρAdxdm = \rho A dx. The weight of this segment is dF=dmg=ρAgdxdF = dm \cdot g = \rho A g dx. The total tension at xx is T(x)=xlρAgdx=ρAg(lx)T(x) = \int_x^l \rho A g dx = \rho A g (l-x).

The stress σ(x)\sigma(x) at position xx is σ(x)=T(x)A=ρg(lx)\sigma(x) = \frac{T(x)}{A} = \rho g (l-x). The strain ϵ(x)\epsilon(x) at position xx is given by ϵ(x)=σ(x)Y(x)\epsilon(x) = \frac{\sigma(x)}{Y(x)}, where Y(x)Y(x) is the Young's modulus at position xx. So, ϵ(x)=ρg(lx)Y(x)\epsilon(x) = \frac{\rho g (l-x)}{Y(x)}.

The elastic energy density u(x)u(x) at position xx is given by u(x)=12σ(x)ϵ(x)u(x) = \frac{1}{2} \sigma(x) \epsilon(x). Substituting the expressions for σ(x)\sigma(x) and ϵ(x)\epsilon(x): u(x)=12(ρg(lx))(ρg(lx)Y(x))=(ρg(lx))22Y(x)u(x) = \frac{1}{2} \left(\rho g (l-x)\right) \left(\frac{\rho g (l-x)}{Y(x)}\right) = \frac{(\rho g (l-x))^2}{2 Y(x)}.

We are given that the elastic energy density u(x)u(x) is the same at every point, so u(x)=u0u(x) = u_0, where u0u_0 is a constant. u0=ρ2g2(lx)22Y(x)u_0 = \frac{\rho^2 g^2 (l-x)^2}{2 Y(x)}.

We need to find how Y(x)Y(x) changes with xx. Rearranging the equation for Y(x)Y(x): Y(x)=ρ2g2(lx)22u0Y(x) = \frac{\rho^2 g^2 (l-x)^2}{2 u_0}.

Since ρ\rho, gg, and u0u_0 are constants, we can write Y(x)=C(lx)2Y(x) = C(l-x)^2, where C=ρ2g22u0C = \frac{\rho^2 g^2}{2 u_0} is a positive constant.

We need to find the graph that represents Y(x)=C(lx)2Y(x) = C(l-x)^2 for xx in the range [0,l][0, l].

  1. At x=0x=0 (top of the rod), Y(0)=C(l0)2=Cl2Y(0) = C(l-0)^2 = Cl^2. This is the maximum value of Young's modulus.
  2. At x=lx=l (bottom of the rod), Y(l)=C(ll)2=0Y(l) = C(l-l)^2 = 0. This is the minimum value of Young's modulus.
  3. The function Y(x)Y(x) is a decreasing function of xx in the range [0,l][0, l].
  4. To determine the concavity, we find the second derivative of Y(x)Y(x) with respect to xx: dYdx=C2(lx)(1)=2C(lx)\frac{dY}{dx} = C \cdot 2(l-x) \cdot (-1) = -2C(l-x). d2Ydx2=2C(1)=2C\frac{d^2Y}{dx^2} = -2C(-1) = 2C. Since C>0C > 0, d2Ydx2>0\frac{d^2Y}{dx^2} > 0. This means the graph of Y(x)Y(x) versus xx is concave up.

Observing the given graphs:

  • Graph (A) shows a linear increase.
  • Graph (B) shows a rapid decrease, resembling an inverse relationship.
  • Graph (C) shows a decrease from a high value to a low value, and the curve is bending upwards (concave up).
  • Graph (D) shows a decrease from a high value to a low value, and the curve is bending downwards (concave down).

Graph (C) correctly represents a function that is decreasing and concave up, matching our derived function Y(x)=C(lx)2Y(x) = C(l-x)^2.