101. Electric Potential Energy of Two Point Charges

101 Electric - q 3 r 23 = k „ q 1 q 2 r 12 q 1 q 3 r 13 q 2 q 3 r 23 #2 Symmetric expression of potential energy U in terms of the potentials

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Electric Potential Energy of Two Point Charges Consider two different perspectives: #1a Electric potential when q 1 is placed: V ( ~ r 2 ) . = V 2 = k q 1 r 12 Electric potential energy when q 2 is placed into potential V 2 : U = q 2 V 2 = k q 1 q 2 r 12 #1b Electric potential when q 2 is placed: V ( ~ r 1 ) . = V 1 = k q 2 r 12 Electric potential energy when q 1 is placed into potential V 1 : U = q 1 V 1 = k q 1 q 2 r 12 . #2 Electric potential energy of q 1 and q 2 : U = 1 2 2 X i =1 q i V i , where V 1 = k q 2 r 12 , V 2 = k q 1 r 12 . 2 z y q 2 r 12 q 1 1 r r tsl101 – p.1/2
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Electric Potential Energy of Three Point Charges #1 Place q 1 , then q 2 , then q 3 , and add all changes in potential energy: U = 0 + k q 1 q 2 r 12 + k q 1 q 3 r 13 + q 2
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Unformatted text preview: q 3 r 23 « = k „ q 1 q 2 r 12 + q 1 q 3 r 13 + q 2 q 3 r 23 « . #2 Symmetric expression of potential energy U in terms of the potentials V i experienced by point charges q 1 : U = 1 2 3 X i =1 q i V i = k „ q 1 q 2 r 12 + q 1 q 3 r 13 + q 2 q 3 r 23 « , where V 1 = k „ q 2 r 12 + q 3 r 13 « , V 2 = k „ q 1 r 12 + q 3 r 23 « , V 3 = k „ q 1 r 13 + q 2 r 23 « . q 2 r 12 q 1 z q 3 r 23 r 13 y tsl102 – p.2/2...
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This note was uploaded on 04/30/2008 for the course PHYS 204 taught by Professor Andrevantonder during the Spring '07 term at Rhode Island.

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101 Electric - q 3 r 23 = k „ q 1 q 2 r 12 q 1 q 3 r 13 q 2 q 3 r 23 #2 Symmetric expression of potential energy U in terms of the potentials

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