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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 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 distance \( d \) is defined as: \[ d = \frac{(\sqrt{x} - 1)}{2} R \] where \( R \) is the radius of the Earth. We know 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 of the Earth. ### Step 1: Write the expression for gravitational acceleration above the surface The acceleration due to gravity at a distance \( d \) above the surface of the Earth is given by: \[ g_{\text{above}} = \frac{GM}{(R + d)^2} \] where \( G \) is the gravitational constant and \( M \) is the mass of the Earth. ### Step 2: Write the expression for gravitational acceleration below the surface The acceleration due to gravity at a distance \( d \) below the surface of the Earth can be expressed as: \[ g_{\text{below}} = \frac{GM'}{(R - d)^2} \] where \( M' \) is the mass of the Earth that is enclosed within a sphere of radius \( R - d \). Since the Earth has uniform density, we can express \( M' \) as: \[ M' = \rho \cdot \frac{4}{3} \pi (R - d)^3 \] where \( \rho \) is the density of the Earth. ### Step 3: Set the two expressions equal to each other Since \( g_{\text{above}} = g_{\text{below}} \), we have: \[ \frac{GM}{(R + d)^2} = \frac{G \cdot \rho \cdot \frac{4}{3} \pi (R - d)^3}{(R - d)^2} \] ### Step 4: Simplify the equation We can cancel \( G \) from both sides: \[ \frac{M}{(R + d)^2} = \frac{\rho \cdot \frac{4}{3} \pi (R - d)^3}{(R - d)^2} \] Now, we can express \( M \) in terms of \( \rho \): \[ M = \rho \cdot \frac{4}{3} \pi R^3 \] Substituting this into the equation gives: \[ \frac{\rho \cdot \frac{4}{3} \pi R^3}{(R + d)^2} = \frac{\rho \cdot \frac{4}{3} \pi (R - d)^3}{(R - d)^2} \] ### Step 5: Cancel common terms We can cancel \( \rho \cdot \frac{4}{3} \pi \) from both sides: \[ \frac{R^3}{(R + d)^2} = \frac{(R - d)^3}{(R - d)^2} \] This simplifies to: \[ \frac{R^3}{(R + d)^2} = (R - d) \] ### Step 6: Cross-multiply and rearrange Cross-multiplying gives: \[ R^3 = (R - d)(R + d)^2 \] Expanding the right side: \[ R^3 = (R - d)(R^2 + 2Rd + d^2) \] ### Step 7: Substitute \( d \) Substituting \( d = \frac{(\sqrt{x} - 1)}{2} R \): \[ R^3 = \left(R - \frac{(\sqrt{x} - 1)}{2} R\right)\left(R^2 + 2R\left(\frac{(\sqrt{x} - 1)}{2} R\right) + \left(\frac{(\sqrt{x} - 1)}{2} R\right)^2\right) \] ### Step 8: Solve for \( x \) After simplifying the equation, we will find the value of \( x \). The solution will yield: \[ x = 5 \] ### Final Answer Thus, the value of \( x \) is: \[ \boxed{5} \]
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