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One model for a certain planet has a core of radius R and mass M surrounded by an outer shell of inner radius R, outer radius 2R, and mass 4M. If M = 2.48 × 1024 kg and R = 1.17 × 106 m, what is the gravitational acceleration of a particle at points (a) R and (b) 3R from the center of the planet?

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(a) 120.8 m/s^2

The gravitational acceleration at a generic distance r from the centre of the planet is


g=(GM')/(r^2)

where

G is the gravitational constant

M' is the mass enclosed by the spherical surface of radius r

r is the distance from the centre

For this part of the problem,


r=R=1.17\cdot 10^6 m

so the mass enclosed is just the mass of the core:


M'=M=2.48\cdot 10^(24)kg

So the gravitational acceleration is


g=((6.67\cdot 10^(-11))(2.48\cdot 10^(24)kg))/((1.17\cdot 10^6 m)^2)=120.8 m/s^2

(b) 67.1 m/s^2

In this part of the problem,


r=3R=3(1.17\cdot 10^6 m)=3.51\cdot 10^6 m

and the mass enclosed here is the sum of the mass of the core and the mass of the shell, so


M'=M+4M=5M=5(2.48\cdot 10^(24)kg)=1.24\cdot 10^(25)kg

so the gravitational acceleration is


g=((6.67\cdot 10^(-11))(1.24\cdot 10^(25)kg))/((3.51\cdot 10^6 m)^2)=67.1 m/s^2

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