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In this region, mass undergo constant acceleration due to gravity, g. Motion with constant g has been dealt with quite extensively in projectile motion.
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In this region, charges undergo constant acceleration a = F/m , where F = qE. Charges in E field behaves like a mass in g field where equations of motion can be applied.The difficulty is direction of acceleration in E field is not obvious as the gfield case.The acceleration is perpendicular the the length of the plates and the direciton is towards the negative plate.
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In this region, charges undergo acceleration a =Bqv/m which is perpendicular to the velocity. The resultant motion is circular and has the value a = v2/r . The Fleming's LHR will be help to determine the centre of the circle(direction of force) given the velocity of the charge and direction of Bfield.
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In this region, charges undergo constant acceleration a = F/m , where F = qE. Charges in E field behaves like a mass in g field where equations of motion can be applied.The difficulty is direction of acceleration in E field is not obvious as the gfield case.The acceleration is perpendicular the the length of the plates and the direciton is towards the negative plate.
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In this region, charges undergo acceleration a =Bqv/m which is perpendicular to the velocity. The resultant motion is circular and has the value a = v2/r . The Fleming's LHR will be help to determine the centre of the circle(direction of force) given the velocity of the charge and direction of Bfield.
