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Chapter 16 – Problem 13

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Given Q=6.00x10 -3 C r=1.00m r=1.00m 2 k=9.0x10 9 N 2 m 2 /C 2. Find Force on the top right charge. Chapter 16 – Problem 13. Given Q=6.00x10 -3 C r=1.00m r=1.00m 2 k=9.0x10 9 N 2 m 2 /C 2. Find Force on the top right charge. Chapter 16 – Problem 13. Given Q=6.00x10 -3 C - PowerPoint PPT Presentation
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Chapter 16 – Problem 13 Given Q=6.00x10 -3 C r=1.00m r=1.00m 2 k=9.0x10 9 N 2 m 2 /C 2 Find Force on the top right charge
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Page 1: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Given

Q=6.00x10-3Cr=1.00mr=1.00m 2 k=9.0x109 N2m2/C2

Find Force on the top

right charge

Page 2: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Given

Q=6.00x10-3Cr=1.00mr=1.00m 2 k=9.0x109 N2m2/C2

Find Force on the top

right charge

Page 3: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Given

Q=6.00x10-3Cr=1.00mr=1.00m 2 k=9.0x109 N2m2/C2

Find Force on the top

right charge

Page 4: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Given

Q=6.00x10-3Cr=1.00mr=1.00m 2 k=9.0x109 N2m2/C2

Find Force on the top

right charge

Page 5: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Given

Q=6.00x10-3Cr=1.00mr=1.00m 2 k=9.0x109 N2m2/C2

Find Force on the top

right charge

Page 6: Chapter 16 – Problem 13

Chapter 16 – Problem 13

F = KQQ / r2 = 9.0x109 N2m2/C2(6.0x10-3)2 / (1.0m)2

Fx=3.24x105N for top left on top right Fy=3.24x105N for bottom right on top right

F=KQQ / r2=9.0x109 N2m2/C2(6.0x10-3)2/(1.0m 2 )2

F=1.62x105N Fx=1.62x105N cos45= 1.15x105N for bottom left on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top right

Page 7: Chapter 16 – Problem 13

Chapter 16 – Problem 13

F = KQQ / r2 = 9.0x109 N2m2/C2(6.0x10-3)2 / (1.0m)2

Fx=3.24x105N for top left on top right Fy=3.24x105N for bottom right on top right

F=KQQ / r2=9.0x109 N2m2/C2(6.0x10-3)2/(1.0m 2 )2

F=1.62x105N Fx=1.62x105N cos45= 1.15x105N for bottom left on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top right

Page 8: Chapter 16 – Problem 13

Chapter 16 – Problem 13

F = KQQ / r2 = 9.0x109 N2m2/C2(6.0x10-3)2 / (1.0m)2

Fx=3.24x105N for top left on top right Fy=3.24x105N for bottom right on top right

F=KQQ / r2=9.0x109 N2m2/C2(6.0x10-3)2/(1.0m 2 )2

F=1.62x105N Fx=1.62x105N cos45= 1.15x105N for bottom left on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top right

Page 9: Chapter 16 – Problem 13

Chapter 16 – Problem 13

F = KQQ / r2 = 9.0x109 N2m2/C2(6.0x10-3)2 / (1.0m)2

Fx=3.24x105N for top left on top right Fy=3.24x105N for bottom right on top right

F=KQQ / r2=9.0x109 N2m2/C2(6.0x10-3)2/(1.0m 2 )2

F=1.62x105N Fx=1.62x105N cos45= 1.15x105N for bottom left on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top right

Page 10: Chapter 16 – Problem 13

Chapter 16 – Problem 13

F = KQQ / r2 = 9.0x109 N2m2/C2(6.0x10-3)2 / (1.0m)2

Fx=3.24x105N for top left on top right Fy=3.24x105N for bottom right on top right

F=KQQ / r2=9.0x109 N2m2/C2(6.0x10-3)2/(1.0m 2 )2

F=1.62x105N Fx=1.62x105N cos45= 1.15x105N for bottom left on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top right

Page 11: Chapter 16 – Problem 13

Chapter 16 – Problem 13

F = KQQ / r2 = 9.0x109 N2m2/C2(6.0x10-3)2 / (1.0m)2

Fx=3.24x105N for top left on top right Fy=3.24x105N for bottom right on top right

F=KQQ / r2=9.0x109 N2m2/C2(6.0x10-3)2/(1.0m 2 )2

F=1.62x105N Fx=1.62x105N cos45= 1.15x105N for bottom left on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top right

Page 12: Chapter 16 – Problem 13

Chapter 16 – Problem 13

F = KQQ / r2 = 9.0x109 N2m2/C2(6.0x10-3)2 / (1.0m)2

Fx=3.24x105N for top left on top right Fy=3.24x105N for bottom right on top right

F=KQQ / r2=9.0x109 N2m2/C2(6.0x10-3)2/(1.0m 2 )2

F=1.62x105N Fx=1.62x105N cos45= 1.15x105N for bottom left on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top right

Page 13: Chapter 16 – Problem 13

Chapter 16 – Problem 13

F = KQQ / r2 = 9.0x109 N2m2/C2(6.0x10-3)2 / (1.0m)2

Fx=3.24x105N for top left on top right Fy=3.24x105N for bottom right on top right

F=KQQ / r2=9.0x109 N2m2/C2(6.0x10-3)2/(1.0m 2 )2

F=1.62x105N Fx=1.62x105N cos45= 1.15x105N for bottom left on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top right

Page 14: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Fx=3.24x105N for top left on top rightFx=1.62x105N cos45= 1.15x105N for bottom left on top rightTotal x = 4.39x105N

Fy=3.24x105N for bottom right on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top rightTotal y = 4.39x105N

Page 15: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Fx=3.24x105N for top left on top rightFx=1.62x105N cos45= 1.15x105N for bottom left on top rightTotal x = 4.39x105N

Fy=3.24x105N for bottom right on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top rightTotal y = 4.39x105N

Page 16: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Fx=3.24x105N for top left on top rightFx=1.62x105N cos45= 1.15x105N for bottom left on top rightTotal x = 4.39x105N

Fy=3.24x105N for bottom right on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top rightTotal y = 4.39x105N

Page 17: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Fx=3.24x105N for top left on top rightFx=1.62x105N cos45= 1.15x105N for bottom left on top rightTotal x = 4.39x105N

Fy=3.24x105N for bottom right on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top rightTotal y = 4.39x105N

Page 18: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Fx=3.24x105N for top left on top rightFx=1.62x105N cos45= 1.15x105N for bottom left on top rightTotal x = 4.39x105N

Fy=3.24x105N for bottom right on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top rightTotal y = 4.39x105N

Page 19: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Fx=3.24x105N for top left on top rightFx=1.62x105N cos45= 1.15x105N for bottom left on top rightTotal x = 4.39x105N

Fy=3.24x105N for bottom right on top right Fy=1.62x105N sin45= 1.15x105N for bottom left on top rightTotal y = 4.39x105N

Page 20: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Total x = 4.39x105N

Total y = 4.39x105N

total (4.39x105N)2 + (4.39x105N)2

Total = 6.2x105N away from the center

Page 21: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Total x = 4.39x105N

Total y = 4.39x105N

total (4.39x105N)2 + (4.39x105N)2

Total = 6.2x105N away from the center

Page 22: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Total x = 4.39x105N

Total y = 4.39x105N

total (4.39x105N)2 + (4.39x105N)2

Total = 6.2x105N away from the center

Page 23: Chapter 16 – Problem 13

Chapter 16 – Problem 13

Total x = 4.39x105N

Total y = 4.39x105N

total (4.39x105N)2 + (4.39x105N)2

Total = 6.2x105N away from the center

Page 24: Chapter 16 – Problem 13

Chapter 16 – Problem 15

GivenQ=1.6x10-19C m=9.11x10-31kg r=.53x10-10m k=9.0x109 N2m2/C2

G=6.67.0x10-11 N2m2/kg2

FindFE

Fg

Page 25: Chapter 16 – Problem 13

Chapter 16 Problem 15

F = KQQ / r2 = 9.0x109 N2m2/C2(1.6x10-19)2

(.53x10-10m)2

F=8.2x10-8N

F = Gmm / r2 = 6.67x10-11 N2m2/C2(9.11x10-31kg)2 (.53x10-10m)2

F=3.6x10-47N

Ratio=8.2x10-8N/3.6x10-47N=2.3x1039 times greater

Page 26: Chapter 16 – Problem 13

Chapter 16 Problem 15

F = KQQ / r2 = 9.0x109 N2m2/C2(1.6x10-19)2

(.53x10-10m)2

F=8.2x10-8N

F = Gmm / r2 = 6.67x10-11 N2m2/C2(9.11x10-31kg)2 (.53x10-10m)2

F=3.6x10-47N

Ratio=8.2x10-8N/3.6x10-47N=2.3x1039 times greater

Page 27: Chapter 16 – Problem 13

Chapter 16 Problem 15

F = KQQ / r2 = 9.0x109 N2m2/C2(1.6x10-19)2

(.53x10-10m)2

F=8.2x10-8N

F = Gmm / r2 = 6.67x10-11 N2m2/C2(9.11x10-31kg)2 (.53x10-10m)2

F=3.6x10-47N

Ratio=8.2x10-8N/3.6x10-47N=2.3x1039 times greater

Page 28: Chapter 16 – Problem 13

Chapter 16 Problem 19

Given

The charge must be placed beyond one of the charges in order for the net force to equal zero

Page 29: Chapter 16 – Problem 13

Chapter 16 Problem 19

GivenQ=5.7x10-6Cr=.25m+xQ2=3.5x10-6C

r2=x

k=9.0x109

N2m2/C2

FindX position a positive or negative particle would experience no force

Page 30: Chapter 16 – Problem 13

Chapter 16 Problem 19

F=KQQ / r2 K(5.7x10–6 C) Q / (.25m + x)2 =K(3.5x10–6 C) Q / x2

(5.7x10–6 C) / (.25m + x)2 =(3.5x10–6 C) / x2

X=.91m beyond the negative charge

The result is independent of the magnitude of the charge and sign of the particle to placed at .91 m

Page 31: Chapter 16 – Problem 13

Chapter 16 Problem 19

F=KQQ / r2 K(5.7x10–6 C) Q / (.25m + x)2 =K(3.5x10–6 C) Q / x2

(5.7x10–6 C) / (.25m + x)2 =(3.5x10–6 C) / x2

X=.91m beyond the negative charge

The result is independent of the magnitude of the charge and sign of the particle to placed at .91 m

Page 32: Chapter 16 – Problem 13

Chapter 16 Problem 19

F=KQQ / r2 K(5.7x10–6 C) Q / (.25m + x)2 =K(3.5x10–6 C) Q / x2

(5.7x10–6 C) / (.25m + x)2 =(3.5x10–6 C) / x2

X=.91m beyond the negative charge

The result is independent of the magnitude of the charge and sign of the particle to placed at .91 m

Page 33: Chapter 16 – Problem 13

Chapter 16 Problem 19

F=KQQ / r2 K(5.7x10–6 C) Q / (.25m + x)2 =K(3.5x10–6 C) Q / x2

(5.7x10–6 C) / (.25m + x)2 =(3.5x10–6 C) / x2

X=.91m beyond the negative charge

The result is independent of the magnitude of the charge and sign of the particle to placed at .91 m

Page 34: Chapter 16 – Problem 13

Chapter 16 Problem 19

F=KQQ / r2 K(5.7x10–6 C) Q / (.25m + x)2 =K(3.5x10–6 C) Q / x2

(5.7x10–6 C) / (.25m + x)2 =(3.5x10–6 C) / x2

X=.91m beyond the negative charge

The result is independent of the magnitude of the charge and sign of the particle to placed at .91 m

Page 35: Chapter 16 – Problem 13

Chapter 16 Problem 19

F=KQQ / r2 K(5.7x10–6 C) Q / (.25m + x)2 =K(3.5x10–6 C) Q / x2

(5.7x10–6 C) / (.25m + x)2 =(3.5x10–6 C) / x2

X=.91m beyond the negative charge

The result is independent of the magnitude of the charge and sign of the particle to placed at .91 m

Page 36: Chapter 16 – Problem 13

Chapter 16 Problem 21

Given q=1.6x10-19C m=9.11x10-31kg E=600 N/C

Find a=?m/s2

Direction=?

Page 37: Chapter 16 – Problem 13

Chapter 16 Problem 21

F=qE= ma F = (1.6x10-19C) (600N/C)=(9.11x10-31kg) a

a=1.04x1014m/s2

Since the charge on the electron is negative and the direction of force and thus the acceleration is opposite to the direction of the electric fieldThe direction of the acceleration is independent of the velocity

Page 38: Chapter 16 – Problem 13

Chapter 16 Problem 21

F=qE= ma F = (1.6x10-19C) (600N/C)=(9.11x10-31kg) a

a=1.04x1014m/s2

Since the charge on the electron is negative and the direction of force and thus the acceleration is opposite to the direction of the electric fieldThe direction of the acceleration is independent of the velocity

Page 39: Chapter 16 – Problem 13

Chapter 16 Problem 21

F=qE= ma F = (1.6x10-19C) (600N/C)=(9.11x10-31kg) a

a=1.04x1014m/s2

Since the charge on the electron is negative and the direction of force and thus the acceleration is opposite to the direction of the electric fieldThe direction of the acceleration is independent of the velocity

Page 40: Chapter 16 – Problem 13

Chapter 16 Problem 21

F=qE= ma F = (1.6x10-19C) (600N/C)=(9.11x10-31kg) a

a=1.04x1014m/s2

Since the charge on the electron is negative and the direction of force and thus the acceleration is opposite to the direction of the electric fieldThe direction of the acceleration is independent of the velocity

Page 41: Chapter 16 – Problem 13

Chapter 16 Problem 21

F=qE= ma F = (1.6x10-19C) (600N/C)=(9.11x10-31kg) a

a=1.04x1014m/s2

Since the charge on the electron is negative and the direction of force and thus the acceleration is opposite to the direction of the electric fieldThe direction of the acceleration is independent of the velocity

Page 42: Chapter 16 – Problem 13

Chapter 16 Problem 21

F=qE= ma F = (1.6x10-19C) (600N/C)=(9.11x10-31kg) a

a=1.04x1014m/s2

Since the charge on the electron is negative and the direction of force and thus the acceleration is opposite to the direction of the electric fieldThe direction of the acceleration is independent of the velocity

Page 43: Chapter 16 – Problem 13

Chapter 16 Problem 27

Given q=1.6x10-19C m=9.11x10-31kg a=125m/s2

FindE=? N/C

Page 44: Chapter 16 – Problem 13

Chapter 16 Problem 27

F=qE= ma F = (1.6x10-19C) E=(9.11x10-31kg) (125m/s2) E=7.12x10-10N/C south

Because the charge on the electron is negative, the direction of force,and thus the acceleration, is opposite to the direction of the electric field, so the electric field is south

Page 45: Chapter 16 – Problem 13

Chapter 16 Problem 27

F=qE= ma F = (1.6x10-19C) E=(9.11x10-31kg) (125m/s2) E=7.12x10-10N/C south

Because the charge on the electron is negative, the direction of force,and thus the acceleration, is opposite to the direction of the electric field, so the electric field is south

Page 46: Chapter 16 – Problem 13

Chapter 16 Problem 27

F=qE= ma F = (1.6x10-19C) E=(9.11x10-31kg) (125m/s2) E=7.12x10-10N/C south

Because the charge on the electron is negative, the direction of force,and thus the acceleration, is opposite to the direction of the electric field, so the electric field is south

Page 47: Chapter 16 – Problem 13

Chapter 16 Problem 27

F=qE= ma F = (1.6x10-19C) E=(9.11x10-31kg) (125m/s2) E=7.12x10-10N/C south

Because the charge on the electron is negative, the direction of force,and thus the acceleration, is opposite to the direction of the electric field, so the electric field is south

Page 48: Chapter 16 – Problem 13

Chapter 16 Problem 27

F=qE= ma F = (1.6x10-19C) E=(9.11x10-31kg) (125m/s2) E=7.12x10-10N/C south

Because the charge on the electron is negative, the direction of force,and thus the acceleration, is opposite to the direction of the electric field, so the electric field is south

Page 49: Chapter 16 – Problem 13

Chapter 16 Problem 27

F=qE= ma F = (1.6x10-19C) E=(9.11x10-31kg) (125m/s2) E=7.12x10-10N/C south

Because the charge on the electron is negative, the direction of force,and thus the acceleration, is opposite to the direction of the electric field, so the electric field is south

Page 50: Chapter 16 – Problem 13

Chapter 16 Problem 30a

.05m

.10m

9.0x10-6C 9.0x10-6C

Find the Electric field strength at (0,.05m)

Given

Page 51: Chapter 16 – Problem 13

Chapter 16 Problem 30a

GivenQ=9.0x10-6Ck=9.0x109 N2m2/C2

r= (.10m)2+(.05m)2

r=.112mtan= .05m/.10m = 26.6o

FindE at (0,.05m)

Page 52: Chapter 16 – Problem 13

Problem 30a

E=kQ r2

E = 9.0x109 N2m2/C2 (9.0x10-6 C)(.112m)2

E=6.48x106 N/C

Page 53: Chapter 16 – Problem 13

Chapter 16 Problem 30a

X-compThe sum of their x components will equal zero

Y comp The sum of their y

components equal twice the y component due to one of the charges

Page 54: Chapter 16 – Problem 13

Chapter 16 Problem 30a

2Fy=2(6.48x106 N/C) sin 26.6

Total Fy =5.8x106N/C

Page 55: Chapter 16 – Problem 13

Chapter 16 Problem 30b

.05m

.05m

9.0x10-6C 9.0x10-6C

Find the Electric field strength at (0,.05m)

Given

.15m

Page 56: Chapter 16 – Problem 13

Chapter 16 Problem 30b

GivenQ=9.0x10-6Ck=9.0x109 N2m2/C2

r= (.05m)2+(.05m)2

r=.0707m = 45o

GivenQ=9.0x10-6Ck=9.0x109 N2m2/C2

r= (.15m)2+(.05m)2

r=.158m tan = .05m/.15m = 18.40

Page 57: Chapter 16 – Problem 13

Problem 30b

E = 9.0x109 N2m2/C2 (9.0x10-6 C)(.0707m)2

E=1.62x107 N/C

Page 58: Chapter 16 – Problem 13

Problem 30b

E = 9.0x109 N2m2/C2 (9.0x10-6 C)(.158m)2

E=3.24x106 N/C

Page 59: Chapter 16 – Problem 13

Chapter 16 Problem 30b

Ey=(1.62x107 N/C) sin 45

EY=1.15x107N/C

Ey=(3.24x106N/C)sin18.4= 1.02x106N/CEy=1.15x107N/C+1.02x106N/C =

Ey=1.25x107N/C

Page 60: Chapter 16 – Problem 13

Chapter 16 Problem 30b

Ex=(1.62x107 N/C) cos 45

Ex=1.15x107N/C

Ex=(3.24x106N/C)cos18.4=3.07x106N/CEx=1.15x107N/C-3.07x106N/C=

Ex=8.43x106N/C

Page 61: Chapter 16 – Problem 13

Chapter 16 Problem 30b

Ex=9.97x106N/C

Ey=1.25x107N/C

E= (8.43x106N/C)2+(1.25x107N/C)2

E=1.5x107N/C

Page 62: Chapter 16 – Problem 13

Problem 31

Page 63: Chapter 16 – Problem 13

Problem 31

K=9.0x109N/CQ=+45.0x10-5CQ=-3.0x10-5C r=.60 m _2=.423m 2Find E field in the center

Page 64: Chapter 16 – Problem 13

Problem 31

E =KQ 9.0x109N/C(+4.5x10-5C) r2 (.423m)2

E=2.26x103 N/CE =KQ 9.0x109N/C(+3.1x10-5C) r2 (.423m)2

E=5.96x105 N/CE=1.46x106N/C diagonally away from +

Page 65: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given Find K.E. = 65.0 keV VB-VA=?kV q = +2e

F/R/S/A KE + PE = O conservation of energy KE + q(VB – VA) = 0

q(VB – VA) = KE

(VB – VA) = KE = -65.0 keV = -32.5kV q +2e

Page 66: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given Find K.E. = 65.0 keV VB-VA=?kV q = +2e

F/R/S/A KE + PE = O conservation of energy KE + q(VB – VA) = 0

q(VB – VA) = KE

(VB – VA) = KE = -65.0 keV = -32.5kV q +2e

Page 67: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given Find K.E. = 65.0 keV VB-VA=?kV q = +2e

F/R/S/A KE + PE = O conservation of energy KE + q(VB – VA) = 0

q(VB – VA) = KE

(VB – VA) = KE = -65.0 keV = -32.5kV q +2e

Page 68: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given Find K.E. = 65.0 keV VB-VA=?kV q = +2e

F/R/S/A KE + PE = O conservation of energy KE + q(VB – VA) = 0

q(VB – VA) = KE

(VB – VA) = KE = -65.0 keV = -32.5kV q +2e

Page 69: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given Find K.E. = 65.0 keV VB-VA=?kV q = +2e

F/R/S/A KE + PE = O conservation of energy KE + q(VB – VA) = 0

q(VB – VA) = KE

(VB – VA) = KE = -65.0 keV = -32.5kV q +2e

Page 70: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given Find K.E. = 65.0 keV VB-VA=?kV q = +2e

F/R/S/A KE + PE = O conservation of energy KE + q(VB – VA) = 0

q(VB – VA) = KE

(VB – VA) = KE = -65.0 keV = -32.5kV q +2e

Page 71: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given Find K.E. = 65.0 keV VB-VA=?kV q = +2e

F/R/S/A KE + PE = O conservation of energy KE + q(VB – VA) = 0

q(VB – VA) = KE

(VB – VA) = KE = -65.0 keV = -32.5kV q +2e

Page 72: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given FindW = 25.0x10-4 J K.E. = 4.82 x 10 -4J VB-VA=?V

q = -7.5x10-6 C

F/R/S/A W = KE + PE

W = KE + q(VB – VA)

W - KE = q(VB – VA)

W - KE = (VB – VA)

q25.0x10-4J – 4.82x10-4J = (VB-VA) = -269 V therefore (VA-VB)

=+269V (-7.50x10-6 C)

Page 73: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given FindW = 25.0x10-4 J K.E. = 4.82 x 10 -4J VB-VA=?V

q = -7.5x10-6 C

F/R/S/A W = KE + PE

W = KE + q(VB – VA)

W - KE = q(VB – VA)

W - KE = (VB – VA)

q25.0x10-4J – 4.82x10-4J = (VB-VA) = -269 V therefore (VA-VB)

=+269V (-7.50x10-6 C)

Page 74: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given FindW = 25.0x10-4 J K.E. = 4.82 x 10 -4J VB-VA=?V

q = -7.5x10-6 C

F/R/S/A W = KE + PE

W = KE + q(VB – VA)

W - KE = q(VB – VA)

W - KE = (VB – VA)

q25.0x10-4J – 4.82x10-4J = (VB-VA) = -269 V therefore (VA-VB)

=+269V (-7.50x10-6 C)

Page 75: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given FindW = 25.0x10-4 J K.E. = 4.82 x 10 -4J VB-VA=?V

q = -7.5x10-6 C

F/R/S/A W = KE + PE

W = KE + q(VB – VA)

W - KE = q(VB – VA)

W - KE = (VB – VA)

q25.0x10-4J – 4.82x10-4J = (VB-VA) = -269 V therefore (VA-VB)

=+269V (-7.50x10-6 C)

Page 76: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given FindW = 25.0x10-4 J K.E. = 4.82 x 10 -4J VB-VA=?V

q = -7.5x10-6 C

F/R/S/A W = KE + PE

W = KE + q(VB – VA)

W - KE = q(VB – VA)

W - KE = (VB – VA)

q25.0x10-4J – 4.82x10-4J = (VB-VA) = -269 V therefore (VA-VB)

=+269V (-7.50x10-6 C)

Page 77: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given FindW = 25.0x10-4 J K.E. = 4.82 x 10 -4J VB-VA=?V

q = -7.5x10-6 C

F/R/S/A W = KE + PE

W = KE + q(VB – VA)

W - KE = q(VB – VA)

W - KE = (VB – VA)

q25.0x10-4J – 4.82x10-4J = (VB-VA) = -269 V therefore (VA-VB)

=+269V (-7.50x10-6 C)

Page 78: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given FindW = 25.0x10-4 J K.E. = 4.82 x 10 -4J VB-VA=?V

q = -7.5x10-6 C

F/R/S/A W = KE + PE

W = KE + q(VB – VA)

W - KE = q(VB – VA)

W - KE = (VB – VA)

q25.0x10-4J – 4.82x10-4J = (VB-VA) = -269 V therefore (VA-VB)

=+269V (-7.50x10-6 C)

Page 79: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given FindW = 25.0x10-4 J K.E. = 4.82 x 10 -4J VB-VA=?V

q = -7.5x10-6 C

F/R/S/A W = KE + PE

W = KE + q(VB – VA)

W - KE = q(VB – VA)

W - KE = (VB – VA)

q25.0x10-4J – 4.82x10-4J = (VB-VA) = -269 V therefore (VA-VB)

=+269V (-7.50x10-6 C)

Page 80: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given FindW = 25.0x10-4 J K.E. = 4.82 x 10 -4J VB-VA=?V

q = -7.5x10-6 C

F/R/S/A W = KE + PE

W = KE + q(VB – VA)

W - KE = q(VB – VA)

W - KE = (VB – VA)

q25.0x10-4J – 4.82x10-4J = (VB-VA) = -269 V therefore (VA-VB)

=+269V (-7.50x10-6 C)

Page 81: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given: Find r = 15.0x10-2m V = ? J q = 4.00x10-6C C k = 9.0x109 N m2 / C2 F/R/S/A V= kq r V = 9.0x109 N m2 / C2 ( 4.00x10-6 C) = 2.40x105 V

15.0x10-2m

Page 82: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given: Find r = 15.0x10-2m V = ? J q = 4.00x10-6C C k = 9.0x109 N m2 / C2 F/R/S/A V= kq r V = 9.0x109 N m2 / C2 ( 4.00x10-6 C) = 2.40x105 V

15.0x10-2m

Page 83: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given: Find r = 15.0x10-2m V = ? J q = 4.00x10-6C C k = 9.0x109 N m2 / C2 F/R/S/A V= kq r V = 9.0x109 N m2 / C2 ( 4.00x10-6 C) = 2.40x105 V

15.0x10-2m

Page 84: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given: Find r = 15.0x10-2m V = ? J q = 4.00x10-6C C k = 9.0x109 N m2 / C2 F/R/S/A V= kq r V = 9.0x109 N m2 / C2 ( 4.00x10-6 C) = 2.40x105 V

15.0x10-2m

Page 85: Chapter 16 – Problem 13

Chapter 17 Problem 7,9,13,15,19

Given: Find r = 15.0x10-2m V = ? J q = 4.00x10-6C C k = 9.0x109 N m2 / C2 F/R/S/A V= kq r V = 9.0x109 N m2 / C2 ( 4.00x10-6 C) = 2.40x105 V

15.0x10-2m

Page 86: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J

Page 87: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J

Page 88: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J

Page 89: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J

Page 90: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J

Page 91: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J

Page 92: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J

Page 93: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J

Page 94: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J

Page 95: Chapter 16 – Problem 13

Chapter 17 Problem 15 Q1 a b Q2

L d

Va = k[(Q1/r1a) + (Q2/r2a)]Va =9x109Nm2/C[((30x10-6C)/.16m)+ (30x10-6C)/.16m))]=3.38x106V

Vb =9x109Nm2/C[((30x10-6C)/.26m)+ (30x10-6C)/.06m))]=5.54x106V

Wab = KE+PE KE = 0

Wab = PE = q(Vb-Va) = .50x10-6C(5.54x106V-3.38x106V)=

Wab = +1.08 J


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