Superfluous
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The problem:
Consider a spherical planet of uniform density \rho. The distance from the planet's center to its surface (i.e., the planet's radius) is R_{p}. An object is located a distance R from the center of the planet, where R\precR_{p} . (The object is located inside of the planet.)
Part A
Find an expression for the magnitude of the acceleration due to gravity, g(R) , inside the planet.
Express the acceleration due to gravity in terms of \rho, R, \pi, and G, the universal gravitational constant.
Part B
Rewrite your result for g(R) in terms of g_{p}, the gravitational acceleration at the surface of the planet, times a function of R.
Express your answer in terms of g_{p}, R, and R_{p}.
My attempt at a solution:
I determined the answer to Part A to be g(R)=(4/3)G\rho \pi R. However, I am uncertain how to find the answer to Part B. I barely even understand what they are asking me to do. I could really use some hints to point me in the right direction.
Thanks.
Consider a spherical planet of uniform density \rho. The distance from the planet's center to its surface (i.e., the planet's radius) is R_{p}. An object is located a distance R from the center of the planet, where R\precR_{p} . (The object is located inside of the planet.)
Part A
Find an expression for the magnitude of the acceleration due to gravity, g(R) , inside the planet.
Express the acceleration due to gravity in terms of \rho, R, \pi, and G, the universal gravitational constant.
Part B
Rewrite your result for g(R) in terms of g_{p}, the gravitational acceleration at the surface of the planet, times a function of R.
Express your answer in terms of g_{p}, R, and R_{p}.
My attempt at a solution:
I determined the answer to Part A to be g(R)=(4/3)G\rho \pi R. However, I am uncertain how to find the answer to Part B. I barely even understand what they are asking me to do. I could really use some hints to point me in the right direction.
Thanks.