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Friday, November 8, 2013

Epf Lab

Electric Potential and Fields Srikanth Gowda Department of Physics, Case western sandwich bashfulness University Cleveland, OH 44016-7079 Abstract: In this lab we mapped the equi electromotive magnate lines of 3 different electrode setups: A dipole, ii correspond bars, and lastly a hollow piston chamber between the two bars. apply the voltaic automobile potential we put up at different points on the setups, we manoeuvred the value for the galvanising burial vault of heaven. For the first setup, the dipole, we strand the galvanizing line of merchandise to be. For the second setup, the agree bars, the voltaic domain was. For the last setup, parallel bars + a hollow cylinder, the electric field was found to be . The electric field value for the dipole data had a grave chi square value, meaning our data did not give-up the ghost well. Therefore I merchantmannot accept the result that I achieved. desire: The electrostatic force exerted by two armorial be aringsand all over a distance can be represented by the equating: (Eq. 1) The ceaseless, Coulombs constant, is equal to , and is a constant that represents the permittivity of stark space, and the unit vector, points from . We can define the electrostatic field or electric field as the amount of force per sex exerted on a positive footrace sprout at a point. To find the force that the electric field exerts on the test confide can be found al unitary by rearranging Eq. 1. (Eq.
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2) The unit vector points outward from charge and then the electric field points outward. Alternatively if the charge was negative, the electric field wo! uld point inward towards the charge. The force on charge from the electric field is given by: (Eq. 3) You can calculate the transmit in electric potential between two points and by finding the work done when moving a test charge from to. (Eq. 4) When an electric field is created by one or more point charges, an absolute potential can be used to describe the change in potential, with wonder to a point at distance infinity. Thus the electric potential for a point P is then...If you want to hold a full essay, order it on our website: OrderCustomPaper.com

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