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A solid sphere of radius R made of a mat...

A solid sphere of radius `R` made of a material of bulk modulus `B` is surrounded by a liquid in a cylindrical container. `A` massless piston of area `A` (the area of container is also `A`) floats on the surface of the liquid. When a mass `M` is placed on the piston to compress the liquid , fractional change in radius of the sphere is `(Mg)/(alpha AB)`. Find the value of `alpha`.

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To solve the problem step by step, we need to analyze the situation involving a solid sphere submerged in a liquid, surrounded by a piston. Here’s the solution: ### Step 1: Understand the System We have a solid sphere of radius \( R \) made of a material with bulk modulus \( B \). The sphere is surrounded by a liquid in a cylindrical container, and a mass \( M \) is placed on a massless piston that floats on the liquid. ### Step 2: Determine the Change in Pressure When the mass \( M \) is placed on the piston, it exerts a force on the liquid, creating a change in pressure (\( \Delta P \)). The change in pressure can be calculated as: \[ \Delta P = \frac{F}{A} = \frac{Mg}{A} \] where \( g \) is the acceleration due to gravity and \( A \) is the area of the piston. ### Step 3: Relate Bulk Modulus to Pressure and Volume Change The bulk modulus \( B \) is defined as: \[ B = -\frac{\Delta P}{\frac{\Delta V}{V}} \] Rearranging gives: \[ \frac{\Delta V}{V} = -\frac{\Delta P}{B} \] ### Step 4: Substitute the Change in Pressure Substituting the expression for \( \Delta P \) into the bulk modulus equation: \[ \frac{\Delta V}{V} = -\frac{\frac{Mg}{A}}{B} = -\frac{Mg}{AB} \] Taking the absolute value, we have: \[ \left| \frac{\Delta V}{V} \right| = \frac{Mg}{AB} \] ### Step 5: Relate Volume Change to Radius Change The volume \( V \) of a sphere is given by: \[ V = \frac{4}{3} \pi R^3 \] The change in volume \( \Delta V \) can be expressed in terms of the change in radius \( \Delta R \): \[ \Delta V = V' - V = \frac{4}{3} \pi (R + \Delta R)^3 - \frac{4}{3} \pi R^3 \] Using the binomial expansion for small changes, we can approximate: \[ \Delta V \approx 4 \pi R^2 \Delta R \] Thus: \[ \frac{\Delta V}{V} \approx \frac{4 \pi R^2 \Delta R}{\frac{4}{3} \pi R^3} = \frac{3 \Delta R}{R} \] ### Step 6: Set the Two Expressions for Volume Change Equal From the previous steps, we have: \[ \frac{Mg}{AB} = \frac{3 \Delta R}{R} \] Rearranging gives: \[ \Delta R = \frac{MgR}{3AB} \] ### Step 7: Find the Fractional Change in Radius The fractional change in radius is given by: \[ \frac{\Delta R}{R} = \frac{Mg}{3AB} \] ### Step 8: Compare with Given Expression The problem states that the fractional change in radius is also given by: \[ \frac{Mg}{\alpha AB} \] By comparing the two expressions: \[ \frac{Mg}{3AB} = \frac{Mg}{\alpha AB} \] This implies: \[ \alpha = 3 \] ### Final Answer Thus, the value of \( \alpha \) is: \[ \alpha = 3 \]

To solve the problem step by step, we need to analyze the situation involving a solid sphere submerged in a liquid, surrounded by a piston. Here’s the solution: ### Step 1: Understand the System We have a solid sphere of radius \( R \) made of a material with bulk modulus \( B \). The sphere is surrounded by a liquid in a cylindrical container, and a mass \( M \) is placed on a massless piston that floats on the liquid. ### Step 2: Determine the Change in Pressure When the mass \( M \) is placed on the piston, it exerts a force on the liquid, creating a change in pressure (\( \Delta P \)). The change in pressure can be calculated as: \[ ...
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