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In a reference frame that is rotating at a constant
In the diagram above, a ball is being thrown by Ann at
point A to Bill at point B with velocity v. The platform is rotating
counter-clockwise. The ball also has a tangential velocity vA =
rA This is not the inertial force named centrifugal force because centrifugal force acts radially outward from the center. This inertial force is acting sidewise. Since F = ma, we can also use the term Coriolis Acceleration. rB - rA = vt v, the radial velocity due to being thrown by Ann sA = vAt sA, the displacement to the side by the ball sB = vBt sB, the displacement to the side by Bill s = sB - sA = ( vB - vA )t s, the displacement behind Bill. How far behind Bill the ball passes. vA = rA s = ( rB - rA ) s = v
s =
acor = 2v
Because the Earth rotates, Coriolis Force has an effect on weather. Without Coriolis Force, wind would flow directly from high pressure areas into low pressure areas. With Coriolis Force, the winds are deflected to the right in the Northern Hemisphere creating counter-clockwise wind patterns around low pressure areas. The winds deflect the opposite direction in the Southern Hemisphere. The Coriolis Force of Earth's rotation, is not a large force. It has minimal effect on dense objects. If a ball is dropped from a tall tower, the displacement to the East does exist, but it is small. The reason it has an effect on weather is the low density of the air added to the large number of individual molecules affected. |