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Question: Copper of fixed volume V is drawn into wire of length $l$. When this wire is subjected to a constant...

Copper of fixed volume V is drawn into wire of length ll. When this wire is subjected to a constant force F, the extension produced in the wire is Δl\Delta l. Which of the following graphs is a straight line ?

A

Δl\Delta l versus 1/l1/l

B

Δl\Delta l versus l2l^2

C

Δl\Delta l versus 1/l21/l^2

D

Δl\Delta l versus ll

Answer

Δl\Delta l versus l2l^2

Explanation

Solution

The Young's modulus (YY) of a material is defined as the ratio of stress to strain: Y=StressStrainY = \frac{\text{Stress}}{\text{Strain}}

For a wire subjected to a tensile force FF, the stress is FA\frac{F}{A}, where AA is the cross-sectional area. The strain is Δll\frac{\Delta l}{l}, where Δl\Delta l is the extension and ll is the original length. So, Y=F/AΔl/l=FlAΔlY = \frac{F/A}{\Delta l/l} = \frac{Fl}{A \Delta l}.

Rearranging this equation to find the extension Δl\Delta l: Δl=FlAY\Delta l = \frac{Fl}{A Y}

We are given that the wire is made from a fixed volume VV of copper. The volume of a wire is given by V=A×lV = A \times l. From this, we can express the cross-sectional area AA in terms of VV and ll: A=VlA = \frac{V}{l}

Substitute this expression for AA into the equation for Δl\Delta l: Δl=Fl(V/l)Y=Fl2VY\Delta l = \frac{Fl}{(V/l)Y} = \frac{Fl^2}{VY}

Since the force FF, the volume VV, and the Young's modulus YY of copper are constant, we can write this relationship as: Δl=Kl2\Delta l = K l^2 where K=FVYK = \frac{F}{VY} is a constant.

This equation shows that the extension Δl\Delta l is directly proportional to the square of the length ll. A graph of Δl\Delta l versus l2l^2 will be a straight line passing through the origin, with the slope equal to the constant KK.

Let's examine the given options:

  1. Δl\Delta l versus 1/l1/l: If we plot Δl\Delta l against 1/l1/l, let x=1/lx = 1/l. Then l=1/xl = 1/x. The relationship becomes Δl=K(1/x)2=K/x2\Delta l = K (1/x)^2 = K/x^2. This is not a linear relationship.
  2. Δl\Delta l versus l2l^2: If we plot Δl\Delta l against l2l^2, let x=l2x = l^2. The relationship becomes Δl=Kx\Delta l = Kx. This is of the form y=mxy = mx, which represents a straight line passing through the origin with slope m=Km=K.
  3. Δl\Delta l versus 1/l21/l^2: If we plot Δl\Delta l against 1/l21/l^2, let x=1/l2x = 1/l^2. Then l2=1/xl^2 = 1/x. The relationship becomes Δl=K(1/x)=K/x\Delta l = K (1/x) = K/x. This is not a linear relationship.
  4. Δl\Delta l versus ll: If we plot Δl\Delta l against ll, let x=lx = l. The relationship becomes Δl=Kx2\Delta l = Kx^2. This is a quadratic relationship, representing a parabola, not a straight line.

Therefore, the graph of Δl\Delta l versus l2l^2 is a straight line.