HW8 - yang (ey942) – oldhomework 08 – Turner –...

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Unformatted text preview: yang (ey942) – oldhomework 08 – Turner – (56705) 1 This print-out should have 13 questions. Multiple-choice questions may continue on the next column or page – find all choices before answering. 001 (part 1 of 4) 10.0 points Two charges are located in the ( x, y ) plane as shown in the figure below. The fields pro- duced by these charges are observed at the origin, p = (0 , 0). The Coulomb constant is 8 . 98755 × 10 9 N · m 2 / C 2 . x y- Q- Q p b a a Use Coulomb’s law to find the x-component of the electric field at p . 1. E x =- 2 k e Q a 2 + b 2 2. E x =- k e Q a ( a 2 + b 2 ) 3 / 2 3. E x = 2 k e Q a ( a 2 + b 2 ) 3 / 2 4. E x =- 2 k e Q a ( a 2 + b 2 ) 3 / 2 5. E x = 4 k e Q a ( a 2 + b 2 ) 3 / 2 6. E x = 2 k e Q a 2 + b 2 7. E x = 0 correct 8. E x =- 4 k e Q a ( a 2 + b 2 ) 3 / 2 9. E x = k e Q a ( a 2 + b 2 ) 3 / 2 Explanation: Let : k e = 8 . 98755 × 10 9 N · m 2 / C 2 .- Q 1- Q 2 p b a a r 1 = radicalBig x 2 1 + y 2 1 = radicalbig a 2 + b 2 . r 2 = radicalBig x 2 2 + y 2 2 = radicalBig (- a ) 2 + b 2 = radicalbig a 2 + b 2 , so r 2 = r 1 = r . θ θ E 1 E 2- Q 1- Q 2 where | sin θ | = b r = b √ a 2 + b 2 | cos θ | = a r = a √ a 2 + b 2 . In the x-direction, the contributions from the two charges are E x 1 =- k e (- Q ) r 2 1 | cos( θ ) | (1) =- k e (- Q ) ( a 2 + b 2 ) a √ a 2 + b 2 = + k e Q a ( a 2 + b 2 ) 3 / 2 E x 2 =- k e (+ Q ) r 2 2 | cos( θ ) | (2) =- k e (+ Q ) ( a 2 + b 2 ) a √ a 2 + b 2 =- k e Q a ( a 2 + b 2 ) 3 / 2 yang (ey942) – oldhomework 08 – Turner – (56705) 2 E x = E x 1 + E x 2 = 0 . 002 (part 2 of 4) 10.0 points Let: V = 0 at infinity. Find the electric potential at p. 1. V y = 4 k e Q a √ a 2 + b 2 2. V y = 4 k e Q √ a 2 + b 2 3. V y = 2 k e Q a √ a 2 + b 2 4. V y =- 4 k e Q √ a 2 + b 2 5. V y =- 4 k e Q a √ a 2 + b 2 6. V y = + 2 k e Q √ a 2 + b 2 7. V y = 0 8. V y =- 2 k e Q √ a 2 + b 2 correct 9. V y =- 2 k e Q a √ a 2 + b 2 Explanation: The potential for a point charge- Q is V = k e- Q r . For the two charges in this problem, we have V 1 = k e- Q √ a 2 + b 2 . V 2 = k e- Q √ a 2 + b 2 . V p = V 1 + V 2 = k e √ a 2 + b 2 [- Q + (- Q )] =- 2 k e Q √ a 2 + b 2 . 003 (part 3 of 4) 10.0 points Find the y-component of the electric field at p. 1. E y =- k e Q b ( a 2 + b 2 ) 3 / 2 2. E y = + k e Q b ( a 2 + b 2 ) 3 / 2 3. E y = + 4 k e Q b ( a 2 + b 2 ) 3 / 2 4. E y =- 4 k e Q b ( a 2 + b 2 ) 3 / 2 5. E y =- 2 k e Q a 2 + b 2 6. E y =- 2 k e Q b ( a 2 + b 2 ) 3 / 2 correct 7. E y = 0 8. E y = + 2 k e Q a 2 + b 2 9. E y = + 2 k e Q b ( a 2 + b 2 ) 3 / 2 Explanation: r = ( x 2 + y 2 ) 1 / 2 = ( a 2 + b 2 ) 1 / 2 and ∂ r ∂y = 1 2 ( y 2 + x 2 )- 1 / 2 · 2 y ∂ V ∂r =- k e + Q r 2 ....
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This note was uploaded on 11/21/2010 for the course PHY 56705 taught by Professor Turner during the Spring '10 term at University of Texas.

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HW8 - yang (ey942) – oldhomework 08 – Turner –...

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