Gravitation vertical mine shaft question

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SUMMARY

The discussion focuses on deriving the gravitational acceleration at the bottom of a vertical mine shaft of depth D, using the formula g = g_{s}(1 - D/R), where g_{s} is the gravitational acceleration at the Earth's surface and R is the Earth's radius. The solution involves applying the gravitational force equation F = GMm/r² and understanding the mass ratio based on density to account for the mass of the Earth below the shaft. The key insight is that only the mass beneath the observer contributes to gravitational attraction, while the mass above does not.

PREREQUISITES
  • Understanding of gravitational force equations, specifically F = GMm/r²
  • Knowledge of volume calculations, particularly V_{S} = (4/3)πr³
  • Familiarity with concepts of density and mass ratios
  • Basic understanding of gravitational acceleration and its variations
NEXT STEPS
  • Study the derivation of gravitational acceleration inside a spherical shell
  • Explore the implications of gravitational potential energy in varying depths
  • Learn about the concept of effective mass in gravitational fields
  • Investigate the relationship between density and gravitational force in planetary bodies
USEFUL FOR

Students in physics, particularly those studying gravitational theory, as well as educators and anyone interested in the mathematical modeling of gravitational forces in varying depths.

homomorphism
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Homework Statement


Show that, at the bottom of a vertical mine shaft dug to depth D, the measured value of g will be

g = g_{s}\left(1-\frac{D}{R}\right)g_{s} being the surface value. Assume that the Earth is a uniform sphere of radius R.

Homework Equations



F = \frac{GMm}{r^{2}}

V_{S} = \frac{4}{3}\pi r^{3}

The Attempt at a Solution



I thought you could just plug in (R-D) in the force equation but when I looked at the solution they did something with a ratio of masses that looked like this:

\frac{M(r)}{\frac{4}{3}\pi r^{3}} = \frac{M}{\frac{4}{3}\pi R^{3}}

where M is the total mass.

Then the solution went on to this:

F = \frac{GM_{E}m}{r^{2}}\left(\frac{\frac{4}{3}\pi r^{3}}{\frac{4}{3}\pi R^{3}}\right)

I don't really understand these last two steps. Can someone please explain what is happening here, and why are they doing a ratio of masses (related by density) and then multiplying by this ratio?
 
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Right, they are figuring out what part of the Earth contributes to the gravity because as you can imagine, if you are a distance D in a mine shaft, the mass of the ground above you is not going to attract you towards the center of the Earth while the ground below you will. So they used a volume ratio to represent the mass of the Earth still "below" you aka between you and the center
 
homomorphism said:

The Attempt at a Solution



I thought you could just plug in (R-D) in the force equation

Unfortunately, it's not quite that simple, since that equation expresses the force outside a sphere of mass M and radius R.

What the solution is doing, which crytoguy is saying in another way, is to compare the gravitational acceleration, g_s, at the Earth's surface, to a faked-up planet which has the same average density of Earth, but is smaller in radius by an amount D.

The value for Earth's surface gravity is g_s = \frac{GM}{R^2}; you can use a similar equation for the alternative planet's surface gravity, g = \frac{GM(r)}{(R-D)^2}, with r = R - D (I am referring to the solution's manual's notation in part of this).

Putting these pieces together will lead to the desired equation.
 

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