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A cylindrical copper rod is reformed to ...

A cylindrical copper rod is reformed to twice its original length with no change in volume. The resistance between its ends before the change was R. Now its resistance will be :

A

8R

B

6R

C

4R

D

2R

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The correct Answer is:
To solve the problem step by step, we need to analyze the changes in the cylindrical copper rod's dimensions and how they affect its resistance. ### Step 1: Understand the relationship between resistance, length, and area The resistance \( R \) of a cylindrical conductor is given by the formula: \[ R = \frac{\rho L}{A} \] where: - \( R \) is the resistance, - \( \rho \) is the resistivity of the material, - \( L \) is the length of the conductor, - \( A \) is the cross-sectional area. ### Step 2: Define the original parameters Let: - The original length of the rod be \( L \). - The original cross-sectional area be \( A \). - The original resistance be \( R \). From the formula, we can express the original resistance as: \[ R = \frac{\rho L}{A} \] ### Step 3: Determine the new length and area after reforming The problem states that the rod is reformed to twice its original length. Therefore, the new length \( L' \) is: \[ L' = 2L \] Since the volume of the rod remains constant, we can express the volume before and after reforming: \[ \text{Original Volume} = A \cdot L \] \[ \text{New Volume} = A' \cdot L' = A' \cdot (2L) \] Setting these two volumes equal gives: \[ A \cdot L = A' \cdot (2L) \] We can cancel \( L \) from both sides (assuming \( L \neq 0 \)): \[ A = 2A' \] Thus, the new cross-sectional area \( A' \) is: \[ A' = \frac{A}{2} \] ### Step 4: Calculate the new resistance Now we can find the new resistance \( R' \) using the new dimensions: \[ R' = \frac{\rho L'}{A'} \] Substituting \( L' \) and \( A' \): \[ R' = \frac{\rho (2L)}{\frac{A}{2}} = \frac{2\rho L \cdot 2}{A} = \frac{4\rho L}{A} \] ### Step 5: Relate the new resistance to the original resistance We know from the original resistance formula that: \[ R = \frac{\rho L}{A} \] Thus, we can express \( R' \) in terms of \( R \): \[ R' = 4 \cdot \frac{\rho L}{A} = 4R \] ### Conclusion The new resistance \( R' \) after reforming the rod is: \[ R' = 4R \]
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