Fred, who is standing on the equator, fires a gun vertically upwards.
Where will the bullet land back on the ground?
Assume there is no wind or air resistance.
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Due to the conservation of angular momentum, the horizontal component of velocity, v x of the bullet will remain constant. Fred also has the same value for his v x . The difference in landing position is due the the change in radius of the circular path undertaken by the bullet.
Angular velocity, ω is given by
ω = r v x ,
(note that v x is the tangential velocity)
∴ ω ∝ r 1
The fact that v x b u l l e t = v x F r e d lets us look purely at scaling relations. Now
θ = ω t
∴ θ ∝ r 1
Where θ is the angular position.
This tells us that as the bullet flies upwards, away from the centre of the Earth, r b u l l e t increases and consequently θ b u l l e t is less compared to θ F r e d due to his smaller r F r e d . Thus if the rotation is in the eastward direction, Fred will advance further over the time interval, and the bullet will be west of him.
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