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A vertical force Facts on the cross-seac...

A vertical force Facts on the cross-seaction of a cylinder body of radius .r. and length L. If Y is young.s modulus and `sigma` = possoing ratio, find the change in volume of the body?

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To find the change in volume of a cylindrical body subjected to a vertical force, we can follow these steps: ### Step 1: Understand the Geometry of the Cylinder The volume \( V \) of a cylinder is given by the formula: \[ V = \pi r^2 L \] where \( r \) is the radius and \( L \) is the length of the cylinder. ### Step 2: Relate Change in Volume to Strain The change in volume \( \Delta V \) can be expressed in terms of the original volume \( V \) and the strains in the radial and longitudinal directions: \[ \frac{\Delta V}{V} = 2 \frac{\Delta r}{r} + \frac{\Delta L}{L} \] where \( \Delta r \) is the change in radius and \( \Delta L \) is the change in length. ### Step 3: Use Poisson's Ratio Poisson's ratio \( \sigma \) relates the change in radius to the change in length: \[ \sigma = -\frac{\Delta r / r}{\Delta L / L} \] From this, we can express \( \frac{\Delta r}{r} \) in terms of \( \Delta L \): \[ \frac{\Delta r}{r} = -\sigma \frac{\Delta L}{L} \] ### Step 4: Substitute into the Volume Change Equation Substituting \( \frac{\Delta r}{r} \) into the volume change equation gives: \[ \frac{\Delta V}{V} = 2 \left(-\sigma \frac{\Delta L}{L}\right) + \frac{\Delta L}{L} \] This simplifies to: \[ \frac{\Delta V}{V} = -2\sigma \frac{\Delta L}{L} + \frac{\Delta L}{L} \] \[ \frac{\Delta V}{V} = \left(1 - 2\sigma\right) \frac{\Delta L}{L} \] ### Step 5: Relate Change in Length to Stress The change in length \( \Delta L \) can be related to the applied force \( F \) using the formula for stress and Young's modulus \( Y \): \[ \text{Stress} = \frac{F}{A} = \frac{F}{\pi r^2} \] \[ \text{Strain} = \frac{\Delta L}{L} = \frac{\text{Stress}}{Y} = \frac{F}{Y \pi r^2} \] Thus, \[ \frac{\Delta L}{L} = \frac{F}{Y \pi r^2} \] ### Step 6: Substitute Back to Find Change in Volume Now substituting \( \frac{\Delta L}{L} \) back into the volume change equation: \[ \frac{\Delta V}{V} = (1 - 2\sigma) \left(\frac{F}{Y \pi r^2}\right) \] Thus, the change in volume \( \Delta V \) can be expressed as: \[ \Delta V = V \cdot \frac{\Delta V}{V} = \pi r^2 L \cdot (1 - 2\sigma) \left(\frac{F}{Y \pi r^2}\right) \] This simplifies to: \[ \Delta V = L \cdot (1 - 2\sigma) \left(\frac{F}{Y}\right) \] ### Final Answer The change in volume of the body is: \[ \Delta V = \frac{L(1 - 2\sigma)F}{Y} \]
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