Change in gravitational potential below the surface of the Earth

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SUMMARY

The gravitational potential below the Earth's surface continues to decrease, becoming more negative as one moves towards the center. The potential is defined by the equation V = -GM/r, where M is the mass enclosed within radius r. As you descend, the mass decreases by a cubic factor while the radius decreases linearly, resulting in a finite negative value for gravitational potential at the center, rather than zero. The gravitational force is zero at the center, but the potential remains negative and finite.

PREREQUISITES
  • Understanding of gravitational potential and force concepts
  • Familiarity with the equation V = -GM/r
  • Basic knowledge of calculus, particularly integrals
  • Concept of mass distribution within spherical bodies
NEXT STEPS
  • Study the derivation of gravitational potential using calculus
  • Explore the implications of mass distribution in non-homogeneous spheres
  • Learn about gravitational potential energy and its applications
  • Investigate the effects of gravitational potential in astrophysics
USEFUL FOR

Students of physics, particularly those studying gravitational theory, as well as educators and anyone interested in understanding the behavior of gravitational potential within celestial bodies.

MBBphys
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Homework Statement


Hi,
Infinitely far away from a mass-->gravitational potential is zero.
As get closer-->becomes negative.
At surface-->it is the smallest value of r, i.e. the radius of the mass, hence the most negative value for gravitational potential.
But as you go below surface of Earth (say Earth is the mass, and the only mass), what happens to the value of gravitational potential as you go below surface of the Earth?

Homework Equations


V=-GM/r

The Attempt at a Solution


I thought that, as the mass decreases by a cubic factor (volume), but the radius decreases by a linear factor, then the gravitational potential would increase (become more positive) by a factor to the power of 2, reaching zero at centre of earth?

Is this right?
Thanks!
 
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Afraid not. Why would the potential be zero at the center ? Gravitation force IS zero there, though.

Compare (897) here with (4.10.3) http://web.mit.edu/8.02t/www/materials/StudyGuide/guide04.pdf
 
BvU said:
Afraid not. Why would the potential be zero at the center ? Gravitation force IS zero there, though.

Compare (897) here with (4.10.3) http://web.mit.edu/8.02t/www/materials/StudyGuide/guide04.pdf
Thanks for your reply. Could you explain why it is not zero? As in, what would it be? A non-zero finite negative value? Infinite? What would it be?
 
MBBphys said:
what would it be?
Equation 897 at BvU's first link answers that. Just put r=0.

Once you move inside the radius of the Earth, the field gets weaker, but it is still directed towards the Earth's centre. So the potential must be still decreasing.
 
MBBphys said:

Homework Statement


Hi,
Infinitely far away from a mass-->gravitational potential is zero.
As get closer-->becomes negative.
At surface-->it is the smallest value of r, i.e. the radius of the mass, hence the most negative value for gravitational potential.
But as you go below surface of Earth (say Earth is the mass, and the only mass), what happens to the value of gravitational potential as you go below surface of the Earth?

Homework Equations


V=-GM/r

The Attempt at a Solution


I thought that, as the mass decreases by a cubic factor (volume), but the radius decreases by a linear factor, then the gravitational potential would increase (become more positive) by a factor to the power of 2, reaching zero at centre of earth?

Is this right?
Thanks!

If you know calculus already, the proper way to solve this would be to express the potential as an integral of the force divided by the test mass:

$$V(r) = -\int_r^\infty\frac{GM(r)}{r^2}dr$$

While you're above the Earth's surface, M is constant and the integral is simply the integral of ##\frac{1}{r^2}##. When you're below you replace M by ##\frac{4}{3}\pi\rho r^3## (with ##\rho## density of the Earth, if we consider it homogeneous, which it isn't but let's not go there). So the integral does not explode at ##r=0## and has instead a finite value, but still, it's not zero.

Without calculus I'm not sure how you can derive the correct formula, but you can realize at least that the rate of change of the potential never changes sign. If the potential is zero at infinity and negative at the surface, it would take a repulsive force to bring it back to zero, and that never happens. Even when you're below the surface all the layers above you merely cancel out their attraction to zero, they don't pull you upwards. So the potential keeps becoming more negative, it simply does so at a slower rate and does not become infinitely negative.
 

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