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A wire of length l is drawn such that it...

A wire of length l is drawn such that its diameter is reduced to half of its original diameler. If the initial resistance of the wire were `10Omega`. its resistance would become

A

`40 Omega`

B

`60Omega`

C

`120Omega`

D

`160Omega`

Text Solution

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The correct Answer is:
To solve the problem step by step, let's analyze the situation given in the question: ### Step 1: Understand the relationship between volume, length, and diameter When a wire is drawn (stretched), its volume remains constant. The volume \( V \) of a cylindrical wire is given by the formula: \[ V = A \cdot l \] where \( A \) is the cross-sectional area and \( l \) is the length of the wire. ### Step 2: Calculate the initial volume of the wire The initial diameter of the wire is \( D \). The cross-sectional area \( A \) of the wire can be calculated as: \[ A = \frac{\pi D^2}{4} \] Thus, the initial volume \( V \) can be expressed as: \[ V = A \cdot l = \frac{\pi D^2}{4} \cdot l \] ### Step 3: Determine the new dimensions after stretching After the wire is drawn, its diameter is reduced to half, so the new diameter \( D' \) is: \[ D' = \frac{D}{2} \] The new cross-sectional area \( A' \) becomes: \[ A' = \frac{\pi (D')^2}{4} = \frac{\pi \left(\frac{D}{2}\right)^2}{4} = \frac{\pi D^2}{16} \] ### Step 4: Set up the equation for constant volume Since the volume remains constant, we can equate the initial and final volumes: \[ \frac{\pi D^2}{4} \cdot l = A' \cdot l' \] Substituting for \( A' \): \[ \frac{\pi D^2}{4} \cdot l = \frac{\pi D^2}{16} \cdot l' \] Cancelling \( \pi D^2 \) from both sides: \[ \frac{l}{4} = \frac{l'}{16} \] Cross-multiplying gives: \[ 16l = 4l' \implies l' = 4l \] This means the new length of the wire is \( 4l \). ### Step 5: Calculate the new resistance The resistance \( R \) of a wire is given by: \[ R = \frac{\rho l}{A} \] where \( \rho \) is the resistivity of the material. For the initial resistance \( R \): \[ R = \frac{\rho l}{\frac{\pi D^2}{4}} = \frac{4\rho l}{\pi D^2} \] Given that \( R = 10 \, \Omega \), we can write: \[ 10 = \frac{4\rho l}{\pi D^2} \] For the new resistance \( R' \): \[ R' = \frac{\rho l'}{A'} = \frac{\rho (4l)}{\frac{\pi D^2}{16}} = \frac{64\rho l}{\pi D^2} \] ### Step 6: Relate the new resistance to the initial resistance Now substituting for \( R \): \[ R' = 64 \cdot \frac{4\rho l}{\pi D^2} = 64 \cdot \left(\frac{\pi D^2}{4}\right) = 64 \cdot 10 \] Thus: \[ R' = 160 \, \Omega \] ### Final Answer The new resistance of the wire after it has been drawn is: \[ \boxed{160 \, \Omega} \]
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