Gravitational Acceleration inside a Planet

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SUMMARY

The discussion focuses on calculating gravitational acceleration inside a spherical planet of uniform density, specifically deriving the expression for acceleration due to gravity, g(R), in terms of the planet's density (ρ), radius (R), and the universal gravitational constant (G). The solution for Part A is established as g(R) = (4/3)GρπR. For Part B, participants are guided to express g(R) in terms of g_p, the gravitational acceleration at the planet's surface, leading to the final expression g(R) = (R * g_p) / R_p, where R_p is the radius of the planet.

PREREQUISITES
  • Understanding of gravitational acceleration and its derivation.
  • Familiarity with the universal law of gravitation.
  • Knowledge of spherical geometry and uniform density concepts.
  • Basic algebra for manipulating equations and substituting variables.
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  • Learn about the implications of uniform density in planetary physics.
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  • Investigate how to manipulate physical equations to express variables in different forms.
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Students studying physics, particularly those focusing on gravitational theory, astrophysics enthusiasts, and educators teaching concepts related to gravity and planetary science.

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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