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If earth has uniform density, and radius...

If earth has uniform density, and radius 'R'. The value of acceleration due to gravity at distance d above the surface is same as the acceleration due to gravity at distance d below the surface. If `d=((sqrtx-1)/(2))R`, then find x.

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To solve the problem, we need to find the value of \( x \) given that the acceleration due to gravity at a distance \( d \) above the surface of the Earth is equal to the acceleration due to gravity at a distance \( d \) below the surface. The distance \( d \) is given as: \[ d = \frac{\sqrt{x} - 1}{2} R \] where \( R \) is the radius of the Earth. ### Step-by-step Solution: 1. **Understanding the Acceleration due to Gravity:** - The acceleration due to gravity at a height \( h \) above the surface of the Earth is given by: \[ g_h = \frac{GM}{(R + h)^2} \] - The acceleration due to gravity at a depth \( d \) below the surface is given by: \[ g_d = \frac{GM'}{(R - d)^2} \] - Here, \( M' \) is the mass of the Earth enclosed within the radius \( R - d \). 2. **Using Uniform Density:** - Since the Earth has uniform density, the mass \( M' \) at depth \( d \) can be expressed as: \[ M' = \rho \cdot \frac{4}{3} \pi (R - d)^3 \] - The total mass \( M \) of the Earth can be expressed as: \[ M = \rho \cdot \frac{4}{3} \pi R^3 \] 3. **Setting Up the Equations:** - The condition states that \( g_h = g_d \): \[ \frac{GM}{(R + d)^2} = \frac{GM'}{(R - d)^2} \] - Cancelling \( G \) from both sides: \[ \frac{M}{(R + d)^2} = \frac{M'}{(R - d)^2} \] 4. **Substituting for \( M' \):** - Substitute \( M' \) in the equation: \[ \frac{M}{(R + d)^2} = \frac{\rho \cdot \frac{4}{3} \pi (R - d)^3}{(R - d)^2} \] - Simplifying gives: \[ \frac{M}{(R + d)^2} = \rho \cdot \frac{4}{3} \pi (R - d) \] 5. **Expressing \( M \) in terms of \( \rho \):** - From the total mass of the Earth: \[ M = \rho \cdot \frac{4}{3} \pi R^3 \] - Substitute this into the equation: \[ \frac{\rho \cdot \frac{4}{3} \pi R^3}{(R + d)^2} = \rho \cdot \frac{4}{3} \pi (R - d) \] - Cancelling \( \rho \cdot \frac{4}{3} \pi \) gives: \[ \frac{R^3}{(R + d)^2} = (R - d) \] 6. **Cross Multiplying:** - Cross multiplying gives: \[ R^3 = (R - d)(R + d)^2 \] 7. **Expanding the Right Side:** - Expanding the right side: \[ R^3 = (R - d)(R^2 + 2Rd + d^2) \] - This expands to: \[ R^3 = R^3 + 2R^2d + Rd^2 - dR^2 - 2d^2R - d^3 \] - Simplifying gives: \[ 0 = 2R^2d + Rd^2 - dR^2 - 2d^2R - d^3 \] 8. **Rearranging the Terms:** - Rearranging leads to: \[ d^3 + (R - 2R^2)d + 2R^2d = 0 \] 9. **Substituting for \( d \):** - Substitute \( d = \frac{\sqrt{x} - 1}{2} R \): \[ \left(\frac{\sqrt{x} - 1}{2} R\right)^3 + (R - 2R^2)\left(\frac{\sqrt{x} - 1}{2} R\right) + 2R^2\left(\frac{\sqrt{x} - 1}{2} R\right) = 0 \] 10. **Solving for \( x \):** - After simplifying and solving, we find that \( x = 5 \). ### Final Answer: \[ x = 5 \]
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