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Variation of g with depth
Intermediate
Inside the Earth, g falls linearly toward the centre.
g' = g(1−d/R)Inside a uniform Earth only the mass inside radius r attracts, so g' = g(1 − d/R), falling linearly to zero at the centre.
At half the radius g' = 4.9 m/s².
Real Earth is denser at the core, so g first slightly increases.
In more detail
Inside a uniform Earth, g decreases linearly with depth, becoming zero at the centre. Only the mass below the point contributes to the pull there.
Real-world uses
- Mines are assessed for gravity changes as depth increases.
- Gravimeters can detect underground voids by small changes in g.
- Geophysicists use the variation of g with depth to infer the density structure of the Earth's interior.
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Frequently asked questions
Is g zero at the centre of the Earth?
Yes, in a uniform-density model, the mass pulling outward cancels the mass pulling inward.
Why does depth reduce g?
Because the mass outside the point at depth contributes nothing to the net pull.
Why does g fall inside the Earth?
Only the mass below you pulls on you, and that mass shrinks as you go deeper, so the net pull weakens.
Related topics in Gravitation & Orbits
Gravitational constant G · Acceleration due to gravity · Variation of g with altitude · Effect of Earth's rotation on g · Gravitational field · Gravitational potential energy