Gravitational Acceleration inside a Planet

AI Thread Summary
The discussion revolves around calculating gravitational acceleration inside a spherical planet of uniform density. For Part A, the acceleration due to gravity is expressed as g(R) = (4/3)GρπR. In Part B, participants are tasked with rewriting this expression in terms of the gravitational acceleration at the planet's surface, g_p, and the planet's radius, R_p. The key to solving Part B involves substituting known values and eliminating constants like G and ρ. Ultimately, the correct expression is derived as g(R) = (R/g_p) * R_p.
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.
 
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They want you to eliminate G, rho etc, and express the ans you got in terms of g at surface.

You do know that M = (4/3)pi*Rp^3*rho. Also, you should know g at surface using law of gravitation. Use all these to eliminate the unwanted stuff.
 
Ok, well I've tried to work this out, but I'm basically just guessing at everything--I'm that clueless. I don't even see how knowing M will help me. I don't know what to do.
 
Superfluous said:
Express your answer in terms of g_{p}, R, and R_{p}.

What the question is asking you to do is to find some function f such that

g(R) = f(g_p,R_p,R)

In other words, somehow replace the G and \rho from the solution already at hand,

g(R) = \frac 4 3 G \pho \pi R

with g_p and R_p. What is g_p?
 
Superfluous said:
Ok, well I've tried to work this out, but I'm basically just guessing at everything--I'm that clueless. I don't even see how knowing M will help me. I don't know what to do.

Put Rp in place of R in the formula you derived in our first post. Remember, g(Rp) is the g_p at the surface. So, you can write g(R) in terms of g_p and R.
 
i'm doing the same question, got the first part right and i got to admit, i still don't get it, i know it has something to do with substiting the value of g_p but and that that can be obtained by using the universal law of gravitation, but after that i am stumped.
 
just worked it out, you got to subsitute formulae and you should end up with R*g_p/R_p
 
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