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A steel wire is suspended vertically fro...

A steel wire is suspended vertically from a rigid support. When loaded with a weight in air, it expands by and when the weight is immersed completely in water, the extension is reduced to `L_(w)`. Then relative done of the material of weight is

A

`(L_(a))/(L_(a) - L_(w))`

B

`(L_(w))/(L_(a))`

C

`(L_(a))/(L_(w))`

D

`(L_(w))/(L_(a) - L_(w))`

Text Solution

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The correct Answer is:
To solve the problem, we will follow these steps: ### Step 1: Understand the Problem We have a steel wire suspended vertically. When a weight is attached to it, the wire extends by \( L_A \) when in air and by \( L_W \) when the weight is submerged in water. We need to find the relative density of the material of the weight. ### Step 2: Write the Expression for Extension in Air The extension of the wire in air can be expressed using Young's modulus: \[ L_A = \frac{F L}{Y A} \] where: - \( L_A \) = extension in air - \( F \) = force applied (weight) - \( L \) = original length of the wire - \( Y \) = Young's modulus of the material - \( A \) = cross-sectional area of the wire ### Step 3: Write the Expression for Extension in Water When the weight is submerged in water, the effective force acting on the wire is reduced due to the buoyant force. The extension in water can be expressed as: \[ L_W = \frac{(W - F_b) L}{Y A} \] where: - \( W \) = weight of the object - \( F_b \) = buoyant force = \( \rho_{water} \cdot V \cdot g \) - \( V \) = volume of the object - \( \rho_{water} \) = density of water The buoyant force can also be expressed as: \[ F_b = \frac{\rho_{water}}{\rho_{object}} W \] Thus, we can write: \[ L_W = \frac{W - \frac{\rho_{water}}{\rho_{object}} W}{Y A} L \] This simplifies to: \[ L_W = \frac{W \left(1 - \frac{\rho_{water}}{\rho_{object}}\right) L}{Y A} \] ### Step 4: Relate the Two Extensions Now, we can relate the two extensions \( L_A \) and \( L_W \): \[ \frac{L_A}{L_W} = \frac{F L}{(W \left(1 - \frac{\rho_{water}}{\rho_{object}}\right) L)} \cdot \frac{Y A}{Y A} \] This simplifies to: \[ \frac{L_A}{L_W} = \frac{F}{W \left(1 - \frac{\rho_{water}}{\rho_{object}}\right)} \] ### Step 5: Find the Relative Density The relative density \( \rho_{relative} \) is defined as: \[ \rho_{relative} = \frac{\rho_{object}}{\rho_{water}} \] From the previous equation, we can rearrange to find: \[ \rho_{relative} = \frac{L_A}{L_A - L_W} \] ### Final Expression Thus, the relative density of the material of the weight is given by: \[ \rho_{relative} = \frac{L_A}{L_A - L_W} \]

To solve the problem, we will follow these steps: ### Step 1: Understand the Problem We have a steel wire suspended vertically. When a weight is attached to it, the wire extends by \( L_A \) when in air and by \( L_W \) when the weight is submerged in water. We need to find the relative density of the material of the weight. ### Step 2: Write the Expression for Extension in Air The extension of the wire in air can be expressed using Young's modulus: \[ ...
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