- #1
AN630078
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- Homework Statement
- Hello, I have found several questions concerning the gravitational field strength of Earth and the equator. I thought them to be rather peculiar since I had not come across any line of questioning similar to this before, therefore, I am uncertain of the methods i have used particularly for question 3. Could anyone comment whether I could improve upon my workings here or offer some further guidance?
Between the poles of Earth and its equator the gravitational field strength varies since the Earth is not perfectly spherical. The measured value of g (and apparent weight) also vary because the Earth is spinning.
1. Taking the radius of the Earth to be 6.4 x 10^6 m, calculate the centripetal force on a 1 kg mass on the equator. (The Earth spins a complete turn in 1 day).
2. The measured value of g at the equator is 9.78, how much would it be if the Earth was not spinning?
3.Using your previous answer for g at the equator, and taking g=9.83 the poles, M = 6.0 x 10^24 kg, and using g = GM/R^2, find out how much further away from the centre of the Earth the equator is than the poles.
- Relevant Equations
- F= mv^2/r
g = GM/R^2
V=2πr/T
1. The centripetal force is equal to F= mv^2/r.
The velocity of the Earth can be found by:
V=2πr/T
T=1 day = 24 hr*60min*60sec=86400 s
v=2π*6.4 x 10^6/86400 s
v=465.4211 ... ~465 ms^-1 to 3.s.f
Therefore, F=1*465/6.4 x 10^6
F=98/1280000=7.265626 *10^-5 ~7.3 *10^-5 N
Would this be correct since it seems incredibly small, although I suppose this is because it is the force acting on a 1kg mass.
2. There would be no change in gravitational field strength since g depends only on the mass of the Earth and our distance from it since g=GM/r^2. Therefore, the measured value at the equator would still be 9.78 N kg^-1. However, there will be a very slight change in the net downward force acting on an object to hold it to the Earth caused by the centripetal acceleration towards the planet's centre by the Earth's rotation. This would disappear if the Earth was no longer rotating.
a=ω2r
a=(2.3*10^−5)2⋅6.37*10^6=3.4*10^−3 ms−2
Which can essentially be neglected as it is on the order of magnitude 3,000 times smaller than g.
3. Would I rearrange g=GM/r^2 in terms of r?
Multiply both sides by r^2: gr^2=GM
Divide both sides by g: r^2 =GM/g
Square root both sides; r= √GM/g
At the equator;
r= √6.67*10^-11*6.0 x 10^24/9.78
r~√4.09*10^13
r=6396893.418 m
At the poles;
r= √6.67*10^-11*6.0 x 10^24/9.83
r~√4.07*10^13
r=6380603.874 m
Difference is distance from centre of the Earth = Distance at equator - distance at poles
6396893.418 - 6380603.874=16289.544 ~ 16300 m to 3.s.f.
The velocity of the Earth can be found by:
V=2πr/T
T=1 day = 24 hr*60min*60sec=86400 s
v=2π*6.4 x 10^6/86400 s
v=465.4211 ... ~465 ms^-1 to 3.s.f
Therefore, F=1*465/6.4 x 10^6
F=98/1280000=7.265626 *10^-5 ~7.3 *10^-5 N
Would this be correct since it seems incredibly small, although I suppose this is because it is the force acting on a 1kg mass.
2. There would be no change in gravitational field strength since g depends only on the mass of the Earth and our distance from it since g=GM/r^2. Therefore, the measured value at the equator would still be 9.78 N kg^-1. However, there will be a very slight change in the net downward force acting on an object to hold it to the Earth caused by the centripetal acceleration towards the planet's centre by the Earth's rotation. This would disappear if the Earth was no longer rotating.
a=ω2r
a=(2.3*10^−5)2⋅6.37*10^6=3.4*10^−3 ms−2
Which can essentially be neglected as it is on the order of magnitude 3,000 times smaller than g.
3. Would I rearrange g=GM/r^2 in terms of r?
Multiply both sides by r^2: gr^2=GM
Divide both sides by g: r^2 =GM/g
Square root both sides; r= √GM/g
At the equator;
r= √6.67*10^-11*6.0 x 10^24/9.78
r~√4.09*10^13
r=6396893.418 m
At the poles;
r= √6.67*10^-11*6.0 x 10^24/9.83
r~√4.07*10^13
r=6380603.874 m
Difference is distance from centre of the Earth = Distance at equator - distance at poles
6396893.418 - 6380603.874=16289.544 ~ 16300 m to 3.s.f.