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Artificial Gravity
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Central Force There is no normal or tension force affecting things in orbit. Like falling bodies that accelerate, a satellite accelerates toward the earth. Gravity is a central force. Satellite centripetal acceleration Earth orbital velocity
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Force on Mass Newton’s law of acceleration applies to orbits. Centripetal acceleration times mass is the force of gravityCentripetal acceleration times mass is the force of gravity The situation is the same for the satellite or any object in the satellite. Satellite or astronaut Earth a F
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Free Fall The net force of an object in circular orbit matches the centripetal acceleration. This is the same for a freely falling object. Velocity does not change the force or acceleration. Earth a F net F net = mg a = g v v
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Weightlessness Objects in free fall exert no normal force. F net = -ma = -mg + F NF net = -ma = -mg + F N If a = g, F N = 0If a = g, F N = 0 The same is true in orbit. F net = ma r = F grav + F NF net = ma r = F grav + F N If a r = F grav /m, F N = 0If a r = F grav /m, F N = 0 Objects in orbit are weightless.
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Spin the Station A spinning station in orbit has a centripetal acceleration of its own. Acceleration is on the inside pointing inward.Acceleration is on the inside pointing inward. There is a corresponding centripetal force for object on the inside wall. Satellite a F
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Station Gravity The centripetal force is like an elevator accelerating upward. F net = ma r = F NF net = ma r = F N The net force must be due to a normal force. Experience as weightExperience as weight If r 2 = g then it matches earth’s gravity.If r 2 = g then it matches earth’s gravity. Satellite a F
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Centrifuge A centrifuge spins to create an artificial gravity. Liquid separation Pilot training Amusement rides
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Gravitron The Gravitron is an amusement ride that uses centripetal force. Rotates at 24 rpm Diameter is 14 m
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Centripetal Correction The spin of the earth creates a centripetal acceleration toward the axis of the earth. The effect is like accelerating down in an elevator. Items weigh less at the equator. a = 2 r
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