SlideShare a Scribd company logo
1 of 13
Chapter 23. The Electric Force                                                       Physics, 6th Edition


                            Chapter 23. The Electric Force

Coulomb's Law

23-1. Two balls each having a charge of 3 ¤ C are separated by 20 mm. What is the force of

       repulsion between them?

                        (9 x 109 N ⋅ m 2 /C2 )(3 x 10-6 C)(3 x 10-6 C)
                   F=                                                  ;    F = 202 N
                                       (20 x 10-3m) 2


23-2. Two point charges of -3 and +4 o C are 12 mm apart in a vacuum. What is the electrostatic

      force between them?

                 (9 x 109 N ⋅ m 2 /C2 )(−3 x 10-6 C)(4 x 10-6 C)
            F=                                                   ;   F = 750 N, attraction
                                  (12 x 10-3 m) 2


23-3. An alpha particle consists of two protons (qe = 1.6 x 10-19 C) and two neutrons (no charge).

       What is the repulsive force between two alpha particles separated by 2 nm?

                                 qα = 2(1.6 x 10-19 C) = 3.2 x 10-19 C

                 (9 x 109 N ⋅ m 2 /C2 )(3.2 x 10-19 C)(3.2 x 10-19 C)
            F=                                                        ;    F = 2.30 x 10-10 N
                                   (2.00 x 10-9 m) 2

23-4. Assume that the radius of the electron's orbit around the proton in a hydrogen atom is

       approximately 5.2 x 10-11 m. What is the electrostatic force of attraction?

                 (9 x 109 N ⋅ m 2 /C2 )(1.6 x 10-19 C)(−1.6 x 10-19 C)
            F=                                                         ;   F = 8.52 x 10-8 N
                                    (5.2 x 10-11m)2

23-5. What is the separation of two -4 a C charges if the force of repulsion between them is

       200 N?

                    kqq '   (9 x 109 N ⋅ m 2 /C2 )(−4 x 10-6 C) 2
                 r=       =                                       ;         r = 26.8 mm
                     F                    200 N



                                                   60
Chapter 23. The Electric Force                                                             Physics, 6th Edition


23-6. Two identical charges separated by 30 mm experience a repulsive force of 980 N. What is

       the magnitude of each charge?

                       kq 2            Fr 2   (980 N)(0.030 m) 2
                  F=        ; q=            =                       ;           q = 9.90    C
                        r2              k      9 x 109 N ⋅ m 2 /C 2



*23-7. A 10     C charge and a -6 r C charge are separated by 40 mm. What is the force between

       them. The spheres are placed in contact for a few moments and then separated again by

       40 mm. What is the new force? Is it attractive or repulsive?

               (9 x 109 N ⋅ m 2 /C2 )(−6 x 10-6 C)(10 x 10-6 C)
            F=                                                  ;         F = 338 N, attraction
                                 (40 x 10-3 m) 2
                                                                                   -6 µC                   10 µC
       When spheres touch, 6 e C of charge are neutralized,                                     0.08 m
       leaving 4 a C to be shared by two spheres, or
                                                                                     2 µC                2 µC
       +2 2 C on each sphere. Now they are again separated.
                                                                                    2 µC                   2 µC
                   (9 x 109 N ⋅ m 2 /C2 )(2 x 10-6 C)(2 x 10-6 C)
                F=                                                ;                             0.08 m
                                     (0.080 m) 2

                               F = 5.62 N, repulsion



*23-8. Two point charges initially attract each other with a force of 600 N. If their separation is

       reduced to one-third of its original distance, what is the new force of attraction?

                                                                            2
                      1                                      r2       r 
                   F∝ 2;       Fr = F r ;
                                1 1
                                   2
                                         2 2
                                            2
                                                    F2 = F1  12  = F1  1  ;    r1 = 3 r2
                     r                                       r2        r2 

                                                2
                                        3r 
                               F2 = F1  2  = 9 F1 ;           F2 = 5400 N
                                        r2 




                                                       61
Chapter 23. The Electric Force                                                         Physics, 6th Edition


The Resultant Electrostatic Force

23-9. A +60 2 C charge is placed 60 mm to the left of a +20           C charge. What is the resultant

       force on a -35 a C charge placed midway between the two charges?
                                                                                    60 mm
             (9 x 109 N ⋅ m 2 /C2 )(60 x 10-6 C)(35 x 10-6 C)
       F13 =                                                         +60 µC         -35 µC         +20 µC
                               (30 x 10-3 m) 2
                                                                        q1            q3                q2
               F13 = 2.10 x 104 N, directed to the left
                                                                             F1                  F2
               (9 x 10 N ⋅ m /C )(20 x 10 C)(35 x 10 C)
                       9      2   2          -6            -6
       F23 =                                            ; F13 = 2.10 x 104 N, directed to right.
                              (30 x 10-3 m) 2

       FR = F13 + F23 = (-2.10 x 104 N) + (0.700 x 104 N);          FR = -1.40 x 104 N, left.


23-10. A point charge of +36 2 C is placed 80 mm to the left of a second point charge of -22

         C. What force is exerted on third charge of +10 c C located at the midpoint?

               (9 x 109 N ⋅ m 2 /C2 )(36 x 10-6 C)(10 x 10-6 C)                        80 mm
       F13 =                                                            +36 µC         10 µC            -22 µC
                                 (40 x 10-3 m) 2
                                                                              q1            q3     F1        q2
               F13 = 2025 N, directed to the right
                                                                                                      F2
               (9 x 10 N ⋅ m /C )(22 x 10 C)(10 x 10 C)
                       9      2   2          -6            -6
       F23 =                                            ; F13 = 1238 N, directed to right.
                              (40 x 10-3 m) 2

                      FR = F13 + F23 = 2025 N + 1238 N;           FR = 3260 N, left.

23-11. For Problem 23-10, what is the resultant force on a third charge of +12 2 C placed

       between the other charges and located 60 mm from the +36               C charge?

               (9 x 109 N ⋅ m 2 /C2 )(36 x 10-6 C)(12 x 10-6 C                       80 mm
       F13 =                                                          +36 µC          q3 = 12 µC        -22 µC
                                (60 x 10-3 m) 2
                                                                                   60 mm                     q2
                                                                         q1                             F1
             (9 x 109 N ⋅ m 2 /C2 )(22 x 10-6 C)(12 x 10-6 C)
       F23 =                                                  ;                        F2
                               (20 x 10-3 m) 2

         Both to right, so FR = F13 + F23 = 1080 N + 5940 N;            F = 7020 N, rightward.



                                                     62
Chapter 23. The Electric Force                                                                Physics, 6th Edition


23-12. A +6 2 C charge is 44 mm to the right of a -8 € C charge. What is the resultant force on

       a -2 a C charge that is 20 mm to the right of the -8            C charge?

             (9 x 109 N ⋅ m 2 /C2 )(8 x 10-6 C)(2 x 10-6 C)                             44 mm
       F13 =                                                           -8 µC                    24 mm 6 µC
                                                                                  q3 = -2 µC
                            (20 x 10-3 m) 2
                                                                                                            q2
                                                                          q1 20 mm                     F1
               (9 x 109 N ⋅ m 2 /C2 )(2 x 10-6 C)(6 x 10-6 C)                            F2
       F23 =                                                  ;
                              (24 x 10-3 m) 2

         Both to right, so FR = F13 + F23 = 360 N + 187.5 N;               F = 548 N, rightward


*23-13. A 64-* C charge is locate 30 cm to the left of a 16-h

       force on a -12 c C charge positioned exactly 50 mm below the 16 s

          s = (30 mm) 2 + (50 mm) 2 = 58.3 mm                              +64 µC 30 mm q2 16 µC
                                                                         q1
                            50 mm                                                   φ
                    tan φ =       ;      φ = 59.0   0

                            30 mm
                                                                                   s
                 (9 x 10 N ⋅ m /C )(64 x 10 C)(12 x 10 C)
                        9      2   2           -6             -6                                      50 mm
         F13 =
                              (58.3 x 10-3 m) 2                                           F1           F2
                   F13 = 2033 N, 59.00 N of W                                                   φ
                                                                                                 q3 = -12 µC
              (9 x 109 N ⋅ m 2 /C2 )(16 x 10-6 C)(12 x 10-6 C)
        F23 =                                                  = 691 N, upward.
                               (50 x 10-3m) 2

                     Fx = 0 – F13 cos 59.00 = -(2033 N) cos 590 ;             Fx = -1047 N

                  Fy = F23 + F13 sin 59.00 = 691 N + (2033 N) sin 590; Fy = 2434 N

                                                                      2434 N
        F = ( −1047 N) 2 + (2434 N) 2 = 2650 N;              tanθ =           ;     N = 66.70 N of W.
                                                                      -1047 N

                       Resultant force: FR = 2650 N, 66.70 N of W (or 113.30)




                                                        63
Chapter 23. The Electric Force                                                            Physics, 6th Edition


*23-14. A charge of +60 nC is located 80 mm above a -40-nC charge. What is the resultant force

       on a -50-nC charge located 45 mm horizontally to the right of the -40-nC charge?
                                                                              +60 µC
       s = (45 mm) 2 + (80 mm) 2 = 91.8 mm                               q1

                               80 mm
                     tan φ =         ;     φ = 60.640
                               45 mm                                                      s
                                                                       80 mm
              (9 x 109 N ⋅ m 2 /C2 )(60 x 10-6 C)(50 x 10-6 C)
        F13 =                                                                            F1
                              (91.8 x 10-3 m) 2                                                         F2
                                                                         q2                     F2
                    F13 = 2564 N, 60.640 N of W                                      45 mm
                                                                         -40 µC                 q3 = -50 µC
                (9 x 109 N ⋅ m 2 /C2 )(40 x 10-6 C)(50 x 10-6 C)
        F23 =                                                    = 8889 N, rightward.
                                  (45 x 10-3 m) 2

          Fx = – F13 cos 60.640 + F23 = - (2564 N) cos 60.640 + 8889 N ;               Fx = 7632 N

                    Fy = +F13 sin 60.640 + 0 = (2564 N) sin 60.640 ;          Fy = 2235 N

                                                      2235 N
       F = (7632 N) 2 + (2235 N) 2 ; tanθ =                  ; FR = 7950 N, 2 = 16.30 N of E.
                                                      7632 N


*23-15. Three point charges q1 = + 8          C, q2 = -4     C, and q3 = +2    C are placed at the corners

       of an equilateral triangle, 80 mm on each side as described by Fig. 23-15. What are the

       magnitude and direction of the resultant force on the +8 e C charge?                                 F2

                (9 x 109 N ⋅ m 2 /C 2 )(4 x 10-6 C)(8 x 10-6 C)                      q1= 8 µC
       F21 =                                                                                         600
                               (80 x 10-3 m) 2                                                        600

                                                                                 80 mm                      80 mm
                  F21 = 45.0 N, 600 S of E                                                       F1

                                                                                q3                      φ
                (9 x 109 N ⋅ m 2 /C 2 )(2 x 10-6 C)(8 x 10-6 C)
       F31 =                                                                               80 mm q = -4 µC
                               (80 x 10-3m) 2                                   +2 µC             2


       F31 = 22.5 N, 600 N of E;           Fx = (22.5 N) cos 600 + (45 N) cos 600 = 33.8 N

                                 Fy = (22.5 N) sin 600 - (45 N) sin 600 = -19.5 N



                                                        64
Chapter 23. The Electric Force                                                      Physics, 6th Edition


                                                                         -19.5 N
*23-15. (Cont.)   F = (33.8 N) 2 + (−19.5 N) 2 = 39.0 N; tanθ =                  ; θ = −300
                                                                         33.8 N

                       Resultant electric force:     FR = 39.0 N, e = 330.00


Challenge Problems

23-16. What should be the separation of two +5-uC charges so that the force of repulsion is 4 N?

                        kqq '   (9 x 109 N ⋅ m 2 /C2 )(5 x 10-6 C) 2
                  r=          =                                      ;    r = 23.7 cm
                         F                   4.00 N



23-17. The repulsive force between two pith balls is found to be 60 h N. If each pith ball carries

       a charge of 8 nC, what is their separation?

                        kqq '   (9 x 109 N ⋅ m 2 /C2 )(8 x 10-9 C) 2
                  r=          =                                      ;   r = 98.0 mm
                         F                60 x 10-6 N



23-18. Two identical unknown charges experience a mutual repulsive force of 48 N when

       separated by 60 mm. What is the magnitude of each charge?

                       kq 2          Fr 2   (48 N)(0.060 m) 2
                  F=        ; q=          =                      ;       q = 4.38   C
                        r2            k     9 x 109 N ⋅ m 2 /C 2



23-19. One object contains an excess of 5 x 1014 electrons and another has a deficiency of 4 x

       1014 electrons. What is the force each exerts on the other if the objects are 30 mm apart?

       Is it attraction or repulsion? ( 1e = 1.6 x 10-19 C, excess = -, deficiency = +. )

      q1 = (5 x 1014 e)(1.6 x 10-19 C/e) = -80 1 C; q2 = (4 x 1014 e)(1.6 x 10-19 C/e) = +64 1 C

           (9 x 109 N ⋅ m 2 /C2 )(80 x 10-6 C)(64 x 10-6 C)
        F=                                                  ;      F = 5.12 x 104 N, attraction
                             (30 x 10-3 m) 2



                                                   65
Chapter 23. The Electric Force                                                               Physics, 6th Edition


23-20. If it were possible to put 1 C of charge on each of two spheres separated by a distance of

       1 m, what would be the repulsive force in newtons.

                           (9 x 109 N ⋅ m 2 /C2 )(1 C)(1 C)
                        F=                                  ;          F = 9 x 109 N !
                                       (1 m) 2

                   The coulomb is a very large unit for electrostatics applications.


23-21. How many electrons must be placed on each of two spheres separated by 4 mm in order

       to produce a repulsive force of one 400 N?

                         kq 2           Fr 2   (400 N)(0.004 m) 2
                    F=        ; q=           =                       ;          q = 843 nC
                          r2             k      9 x 109 N ⋅ m 2 /C 2

                                            1e     
                     q = 843 x 10-9 C          -19 ;          q = 5.27 x 1012 electrons
                                       1.6 x 10 C 


23-22. A –40-nC charge is placed 40 mm to the left of a +6-nC charge. What is the resultant

       force on a –12-nC charge place 8 mm to the right of the +6-nC charge?
                                                                                                         q3 = -12 nC
             (9 x 109 N ⋅ m 2 /C2 )(40 x 10-9 C)(12 x 10-9 C)                                 6 nC
        F1 =                                                           -40 nC                            8 mm
                               (48 x 10-3 m) 2                                    40 mm
                                                                           q1                  q2
             (9 x 109 N ⋅ m 2 /C2 )(6 x 10-9 C)(12 x 10-9 C)                                                      F1
        F2 =                                                 ;                                      F2
                               (8 x 10-3 m) 2

          Both to right, so FR = F1 + F2 = 1.88 mN – 10.1 mN;                 F = -8.25 mN, leftward


23-23. A 5-2 C charge is placed 6 cm to the right of a 2-g C charge. What is the resultant force

       on a –9 nC charge placed 2 cm to the left of the 2-r C charge?

               (9 x 109 N ⋅ m 2 /C2 )(9 x 10-9 C)(2 x 10-6 C)         -9 nC      2 µC                     5 µC
        F1 =                                                                                 6 cm
                               (2 x 10-2 m) 2
                                                                          2 cm    q1                     q2
                       F1 = +405 mN, to right                                           F1
                                                                                   F2


                                                      66
Chapter 23. The Electric Force                                                                Physics, 6th Edition


                      (9 x 109 N ⋅ m 2 /C2 )(5 x 10-6 C)(9 x 10-9 C)
               F2 =                                                  ;    F2 = +63.3 mN, to right
                                      (8 x 10-2 m) 2

                       Resultant force:       FR = 405 mN + 63.3 mN;             FR = 468 mN


23-24. An equal number of electrons is placed on two metal spheres 3.0 cm apart in air. How

        many electrons are on each sphere if the resultant force is 4500 N?

                         kq 2              Fr 2   (4500 N)(0.03 m) 2
                       F= 2 ; q=                =                       ;         q = 21.2    C
                          r                 k      9 x 109 N ⋅ m 2 /C 2

                                                1e     
                        q = 21.2 x 10-6 C          -19 ;       q = 1.33 x 1014 electrons
                                           1.6 x 10 C 


23-25. A 4-nC charge is placed on a 4-g sphere that is free to move. A fixed 10-n C point

        charge is 4 cm away. What is the initial acceleration of the 4-o C charge?

                             (9 x 109 N ⋅ m 2 /C2 )(4 x 10-9 C)(10 x 10-6 C)
                      F2 =                                                   ;    F2 = 225 mN
                                               (4 x 10-2 m) 2

                                           F 0.225 N
                                      a=    =                    a = 56.2 m/s2
                                           m 0.004 kg


*23-26. What is the resultant force on a +2 * C charge an equal distance of 60 mm from each of

        two –4-g C charges that are 80 mm apart in air?                                   q1= 2 µC
                                40 mm                                                                     φ
                      tan φ =         ;     φ = 48.20                                        F1                   F2
                                60 mm
                                                                                    60 mm                         60 mm
             (9 x 109 N ⋅ m 2 /C2 )(4 x 10-6 C)(2 x 10-6 C)                          q3                       φ
        F2 =
                            (60 x 10-3 m) 2
                                                                                     -4 µC                    q2 = -4 µC
                  F2 = 20.0 N, 48.20 S of E                                                       40 mm

               (9 x 109 N ⋅ m 2 /C2 )(2 x 10-6 C)(4 x 10-6 C)
        F1 =                                                  ;      F1 = 20.0 N, 48.20 S of W
                              (60 x 10-3 m) 2



                                                          67
Chapter 23. The Electric Force                                                               Physics, 6th Edition


*23-26. (Cont.)    Fx = (20 N) cos 48.20 + (20 N) cos 48.20 = 13.33 N - 13.33 N; Fx = 0

                  Fy = (20 N) sin 48.20 + (20 N) sin 48.20 = 14.9 N + 14.9 N;                 Fy = -29.8 N

                                Resultant force: FR = 29.8 N, downward


*23-27. Two charges of +25 and +16 * C are 80 mm apart. A third charge of +60 á C is placed

        between the other charges 30 mm from the +25 i C charge. Find the resultant force on

        the third charge?
                                                                                          80 mm
            (9 x 10 N ⋅ m /C )(60 x 10 C)(25 x 10 C)
                    9       2    2            -6               -6        25 µC       q3 = 60 µC            16 µC
       F1 =
                           (30 x 10-3 m) 2                                                                      q2
                                                                              q1 30 mm            50 mm

                                                                               F2                          F1
             F1 = 15 kN, directed to the right

            (9 x 109 N ⋅ m 2 /C2 )(60 x 10-6 C)(16 x 10-6 C)
       F2 =                                                  ; F13 = 3.46 kN, directed to left.
                              (50 x 10-3 m) 2

                  FR = F1 + F2 = 15 kN + 3.46 kN);                  FR = 11.5 kN, right.


*23-28. A 0.02-g pith ball is suspended freely. The ball is given a charge of +20 l C and placed

         0.6 m from a charge of +50

                   (9 x 109 N ⋅ m 2 /C2 )(20 x 10-6 C)(50 x 10-6 C)
              F=                                                    ;         F = 25.0 N
                                      (0.600 m) 2

                                     F   25.0 N
                            a=         =           ;           a = 1.25 x 106 m/s
                                     m 2 x 10-5 kg


*23-29. A 4 * C charge is located 6 cm from an 8 w

         two charges will the resultant force be zero?
                                                                                   F1 = F2           8 µC
                                                                      4 µC
                                     kq3q1    kq3 q2
                     F1 = F2 ;             =                                   x          6 cm - x
                                      x 2
                                             (6 − x ) 2                  q2                               q1
                                                                                     q3




                                                          68
Chapter 23. The Electric Force                                                                  Physics, 6th Edition


                                        q1       q2                  q 
                           F1 = F2 ;        =           ;      x 2 =  1  (6 − x) 2
                                        x 2
                                              (6 − x) 2               q2 

                                                     q1               4 µC
      Take square root of both sides:         x=        (6 - x) =          (6 - x);       x = 0.707(6 - x)
                                                     q2               8 µC

                    Solving for x, we obtain: x = 2.49 cm from 4-o C charge


*23-30. A charge of +8 nC is placed 40 mm to the left of a –14 nC charge. Where should a third

         charge be placed if it is to experience a zero resultant force?

         Considering the sign of the charges and                         F1 = F2                          -14 nC
                                                                                         8 nC
         their magnitudes, the charge must be to the
                                                                                   x             40 mm
         left of the 8 nC charge as shown.                               q3              q1                  q2

                        kq3 q1     kq3 q2                        q1       q2                   q 
            F1 = F2 ;          =                   F1 = F2 ;         =             ;     x 2 =  1  (40 + x ) 2
                         x 2
                                 (40 + x) 2                      x 2
                                                                       (40 + x ) 2              q2 
         Take square root of both sides:



               q1             8 nC
         x=       (40 + x) =       (40 + x); x = 0.756(40+ x)
               q2            14 nC

                   Solving for x, we obtain:         x = 124 mm left of 8 nC charge.


*23-31. A +16-* C charge is 80 mm to the right of a +9 t C. Where should a third charge be

         placed so that the resultant force is zero?                                   F1 = F2
                                                                         9 µC                            +16 µC
                                 kq3q1     kq3 q2                                 x
                    F1 = F2 ;          =                                                      80 mm - x
                                  x 2
                                         (80 − x ) 2                    q1               q3                  q2

                                       q1       q2                   q 
                          F1 = F2 ;        =            ;      x 2 =  1  (80 − x ) 2
                                       x 2
                                             (80 − x) 2               q2 

                                                   q1             9 µC
    Take square root of both sides:      x=           (80 - x) =        (80 - x); x = 0.750(80 - x)
                                                   q2            16 µ C



                                                       69
Chapter 23. The Electric Force                                                          Physics, 6th Edition


                   Solving for x, we obtain: x = 34.3 mm from 9-o C charge
*23-32. Two 3-g spheres are suspended from a common point with two 80 mm light silk threads

         of negligible mass. What charge must be placed on each sphere if their final positions

         are 50 mm apart?
                                                                                        T             80 mm
                       25 mm                                                   F                 φ       F
             cos φ =         ;     φ = 71.80       Ty = T sin φ = mg
                       80 mm
                                                                                   mg                  mg
                    mg     (3 x 10-3 kg)(9.8 m/s 2 )                                         25 mm
              T=         =                           ;   T = 30.9 mN
                   sin φ          sin 71.80
            Tx = T cos 71.80 = (30.9 mN) cos 71.80;            Tx = 9.67 mN;       ΣFx = 0:          F = Tx

            kq 2                         Fr 2   (9.67 x 10-3 N)(50 x 10-3m) 2
         F = 2 = 9.67 mN;          q=         =                               ;               q = 51.8 nC
             r                            k          9 x 109 N ⋅ m 2 /C2



Critical Thinking Questions

*23-33. A small metal sphere is given a charge of +40 h C, and a second sphere 8 cm away is

       given a charge of –12 s C. What is the force of attraction between them? If the two

       spheres are allowed to touch and are then again placed 8 cm apart, what new electric

       force exists between them? Is it attraction or repulsion?

                (9 x 109 N ⋅ m 2 /C2 )(12 x 10-6 C)(40 x 10-6 C)
           F=                                                    ;   F = 675 N, attraction
                                   (0.080 m) 2
                                                                         40 µC                       -12 µC
       When spheres touch, 6 4 C of charge are neutralized,
                                                                                        0.08 m
       leaving 28 l C to be shared by two spheres, or
                                                                          14 µC                  14 µC
       +14 t C on each sphere. Now they are again separated:
                                                                          14 µC                       14 µC
                                                                                            0.08 m
          (9 x 109 N ⋅ m 2 /C2 )(14 x 10-6 C)(14 x 10-6 C)
       F=                                                  ;
                             (0.080 m) 2




                                                   70
Chapter 23. The Electric Force                                                              Physics, 6th Edition


                                 F = 276 N, repulsion



*23-34. The total charge on two metal spheres 50 mm apart is 80 * C. If they repel each other

        with a force of 800 N, what is the charge on each sphere?                        50 mm
                                                                                  q1                     q2
                    q1 + q2 = 80 q C;       q2 = 80 q C – q1

              kq1q2 kq1 (80 µ C - q1 )             kq1 (80µ C ) − kq12         Fr 2
        F=         =                   ;      F=                       ;            = (80 µ C)q1 − q12
               r2          r2                             r2                    k

       (800 N)(50 x 10-3 m) 2
                                = (80 µ C)q1 − q12 ;       q12 – (80 x 10-6 C)q1+ 222 x 10-12 C2 = 0
         (9 x 109 N ⋅ m 2 /C2 )

          Solve the quadratic equation with a = 1, b = - 80 x 10-6, and c = 222 x 10-12

                                   q1 = 77.1 0 C    and q1 = 2.89 0 C

        Now q2 = 80         C – q1 yields the following : q2 = 2.89 = C and q2 = 77.1 n C

                        Thus, one charge is 77.1       C and the other is 2.89 i C


*23-35. Four small spheres are each given charges of q = +20 * C and placed at the corners of a

       square with sides of length 6 cm. Show that the resultant force on each charge has a

       magnitude equal to 1914 N. What is the direction of the force? What will change if the

       charges are each q = -20       C? (Like charges repel, so sign doesn’t matter.) F1                         F2
                                                                                                          φ
                                                                           q           6 cm
               R = (6 cm) + (6 cm) = 8.485 cm
                             2          2
                                                                                                              F1

              (9 x 109 N ⋅ m 2 /C2 )(20 x 10-6 C)(20 x 10-6 C)
       F1 =                                                           6 cm
                                (6 x 10-2 m) 2                                          R                6 cm

              (9 x 109 N ⋅ m 2 /C2 )(20 x 10-6 C)(20 x 10-6 C)                     φ
       F2 =
                            (8.485 x 10-2 m) 2                         q                                      q
                                                                                       6 cm
                   F1 = 1000 N;      F2 = 500 N; For a square, the angle φ = 450

       Fx = (1000 N) + (500 N) cos 450 + 0 = 1354 N; Fy = 1000 N + (500 N) sin 450 = 1354 N


                                                     71
Chapter 23. The Electric Force                                                                       Physics, 6th Edition


               F = (1354 N) 2 + (1354 N) 2 ;          F = 1914 N, 450        away from center.

*23-36. Two charges q1 and q2 are separated by a distance r. They experience a force F at this

         distance. If the initial separation is decreased by only 40 mm, the force between the

         two charges is doubled. What was the initial separation?
                                                                                        F            x             F
          2kq1q2        kq1q2               2            1                     q1                                          q2
                 =                ;             =
            x 2
                   ( x − 40 mm) 2           x 2
                                                  ( x − 40 mm) 2
                                                                                                     x – 40 mm
           2                  2
         x = 2(x – 40 mm)         Take square root of both sides:
                                                                                            q1           2F        2F q2
                x = 1.414(x – 40 mm);           x = 137 mm


*23-37. Two 8-g pith balls are suspended from silk threads 60 cm long and attached to a

         common point. When the spheres are given equal amounts of negative charge, the balls

         come to rest 30 cm apart. Calculate the magnitude of the charge on each pith ball.

                          0.15 m
                cos φ =          ;        φ = 75.50       Ty = T sin φ = mg                      T
                          0.60 m                                                                                   0.6 m
                                                                                    F                         φ        F
                                     -3               2
                     mg     (8 x 10 kg)(9.8 m/s )
               T=         =                       ;            T = 81.0 mN
                    sin φ          sin 75.50                                            mg                          mg
                                                                                                         0.15 m

         Tx = T cos 71.80 = (81.0 mN) cos 75.50;                Tx = 20.25 mN;              ΣFx = 0:              F = Tx

             kq 2                              Fr 2   (2.025 x 10-4 N)(0.30 m) 2
          F = 2 = 20.25 mN;               q=        =                            ;                       q = -450 nC
              r                                 k         9 x 109 N ⋅ m 2 /C2




                                                          72

More Related Content

What's hot

Problemas del Capítulo II de Física Iii
Problemas del Capítulo II de Física IiiProblemas del Capítulo II de Física Iii
Problemas del Capítulo II de Física Iiiguestf39ed9c1
 
147110756 march-2005
147110756 march-2005147110756 march-2005
147110756 march-2005homeworkping3
 
Thermodynamics problems
Thermodynamics problemsThermodynamics problems
Thermodynamics problemsYuri Melliza
 
Trigonometric Problems
Trigonometric ProblemsTrigonometric Problems
Trigonometric Problemsaluahp
 
PROBLEMAS RESUELTOS (45) DEL CAPÍTULO II DE LABORATORIO DE FÍSICA II - TIPPENS
PROBLEMAS RESUELTOS (45) DEL CAPÍTULO II DE LABORATORIO DE FÍSICA II - TIPPENSPROBLEMAS RESUELTOS (45) DEL CAPÍTULO II DE LABORATORIO DE FÍSICA II - TIPPENS
PROBLEMAS RESUELTOS (45) DEL CAPÍTULO II DE LABORATORIO DE FÍSICA II - TIPPENSLUIS POWELL
 
Contemporary arts in the Philippines - American Era
Contemporary arts in the Philippines - American EraContemporary arts in the Philippines - American Era
Contemporary arts in the Philippines - American EraBelayaDeniseLykaRose
 
Ch19 Electric Potential Energy and Electric Potential
Ch19 Electric Potential Energy and Electric PotentialCh19 Electric Potential Energy and Electric Potential
Ch19 Electric Potential Energy and Electric PotentialScott Thomas
 
Simple Stress: Normal Stress
Simple Stress: Normal StressSimple Stress: Normal Stress
Simple Stress: Normal StressLk Rigor
 
BEF 23803 - Lesson 3 - Balanced Delta Load Thre-Phase Systems.ppt
BEF 23803 - Lesson 3 - Balanced Delta Load Thre-Phase Systems.pptBEF 23803 - Lesson 3 - Balanced Delta Load Thre-Phase Systems.ppt
BEF 23803 - Lesson 3 - Balanced Delta Load Thre-Phase Systems.pptLiewChiaPing
 
Vector mechanics for engineers statics 7th chapter 5
Vector mechanics for engineers statics 7th chapter 5 Vector mechanics for engineers statics 7th chapter 5
Vector mechanics for engineers statics 7th chapter 5 Nahla Hazem
 
Electromagnetic theory EMT lecture 1
Electromagnetic theory EMT lecture 1Electromagnetic theory EMT lecture 1
Electromagnetic theory EMT lecture 1Ali Farooq
 
Simple and Compound Interest
Simple and Compound InterestSimple and Compound Interest
Simple and Compound InterestHector Tibo
 
Capacitance
CapacitanceCapacitance
Capacitancestooty s
 

What's hot (20)

Problemas del Capítulo II de Física Iii
Problemas del Capítulo II de Física IiiProblemas del Capítulo II de Física Iii
Problemas del Capítulo II de Física Iii
 
147110756 march-2005
147110756 march-2005147110756 march-2005
147110756 march-2005
 
Anschp32
Anschp32Anschp32
Anschp32
 
Engineering Economics
Engineering EconomicsEngineering Economics
Engineering Economics
 
70148
70148 70148
70148
 
Thermodynamics problems
Thermodynamics problemsThermodynamics problems
Thermodynamics problems
 
Trigonometric Problems
Trigonometric ProblemsTrigonometric Problems
Trigonometric Problems
 
PROBLEMAS RESUELTOS (45) DEL CAPÍTULO II DE LABORATORIO DE FÍSICA II - TIPPENS
PROBLEMAS RESUELTOS (45) DEL CAPÍTULO II DE LABORATORIO DE FÍSICA II - TIPPENSPROBLEMAS RESUELTOS (45) DEL CAPÍTULO II DE LABORATORIO DE FÍSICA II - TIPPENS
PROBLEMAS RESUELTOS (45) DEL CAPÍTULO II DE LABORATORIO DE FÍSICA II - TIPPENS
 
Contemporary arts in the Philippines - American Era
Contemporary arts in the Philippines - American EraContemporary arts in the Philippines - American Era
Contemporary arts in the Philippines - American Era
 
Ch19 Electric Potential Energy and Electric Potential
Ch19 Electric Potential Energy and Electric PotentialCh19 Electric Potential Energy and Electric Potential
Ch19 Electric Potential Energy and Electric Potential
 
Factors affecting resistance
Factors affecting resistanceFactors affecting resistance
Factors affecting resistance
 
Friction full
Friction fullFriction full
Friction full
 
Simple Stress: Normal Stress
Simple Stress: Normal StressSimple Stress: Normal Stress
Simple Stress: Normal Stress
 
BEF 23803 - Lesson 3 - Balanced Delta Load Thre-Phase Systems.ppt
BEF 23803 - Lesson 3 - Balanced Delta Load Thre-Phase Systems.pptBEF 23803 - Lesson 3 - Balanced Delta Load Thre-Phase Systems.ppt
BEF 23803 - Lesson 3 - Balanced Delta Load Thre-Phase Systems.ppt
 
12 transformer
12 transformer12 transformer
12 transformer
 
Vector mechanics for engineers statics 7th chapter 5
Vector mechanics for engineers statics 7th chapter 5 Vector mechanics for engineers statics 7th chapter 5
Vector mechanics for engineers statics 7th chapter 5
 
Electromagnetic theory EMT lecture 1
Electromagnetic theory EMT lecture 1Electromagnetic theory EMT lecture 1
Electromagnetic theory EMT lecture 1
 
Simple and Compound Interest
Simple and Compound InterestSimple and Compound Interest
Simple and Compound Interest
 
Anschp38
Anschp38Anschp38
Anschp38
 
Capacitance
CapacitanceCapacitance
Capacitance
 

Viewers also liked

Viewers also liked (20)

Anschp22
Anschp22Anschp22
Anschp22
 
Anschp21
Anschp21Anschp21
Anschp21
 
Anschp19
Anschp19Anschp19
Anschp19
 
Anschp18
Anschp18Anschp18
Anschp18
 
Anschp34
Anschp34Anschp34
Anschp34
 
Anschp39
Anschp39Anschp39
Anschp39
 
Anschp26
Anschp26Anschp26
Anschp26
 
Anschp16
Anschp16Anschp16
Anschp16
 
Anschp17
Anschp17Anschp17
Anschp17
 
Anschp36
Anschp36Anschp36
Anschp36
 
Anschp20
Anschp20Anschp20
Anschp20
 
Anschp35
Anschp35Anschp35
Anschp35
 
Anschp37
Anschp37Anschp37
Anschp37
 
Electricity and magnetism 1
Electricity and magnetism 1Electricity and magnetism 1
Electricity and magnetism 1
 
A bright city
A bright city A bright city
A bright city
 
Journal of Family Life
Journal of Family LifeJournal of Family Life
Journal of Family Life
 
Short introduction TMS Cloud Based Mobile Marketing 2014
Short introduction TMS Cloud Based Mobile Marketing 2014Short introduction TMS Cloud Based Mobile Marketing 2014
Short introduction TMS Cloud Based Mobile Marketing 2014
 
G ao f_pres.cliffsnotes
G ao f_pres.cliffsnotesG ao f_pres.cliffsnotes
G ao f_pres.cliffsnotes
 
Direct access
Direct accessDirect access
Direct access
 
actividad 12
actividad 12actividad 12
actividad 12
 

Similar to Anschp23

Problemas (13 Pág. - 37 Probl.) de Carga Eléctrica y Ley de Coulomb Tippens
Problemas (13 Pág. - 37 Probl.) de Carga Eléctrica y Ley de Coulomb   TippensProblemas (13 Pág. - 37 Probl.) de Carga Eléctrica y Ley de Coulomb   Tippens
Problemas (13 Pág. - 37 Probl.) de Carga Eléctrica y Ley de Coulomb TippensLUIS POWELL
 
Problemas (16 Págs. - 42 Probl.) del Capítulo II de Física II
Problemas (16 Págs. - 42 Probl.) del Capítulo II de Física IIProblemas (16 Págs. - 42 Probl.) del Capítulo II de Física II
Problemas (16 Págs. - 42 Probl.) del Capítulo II de Física IILUIS POWELL
 
Tutorial solutions 2010
Tutorial solutions 2010Tutorial solutions 2010
Tutorial solutions 2010Sufi Sulaiman
 
626 pages
626 pages626 pages
626 pagesJFG407
 
Latihan soal jawab fentrans
Latihan soal jawab fentransLatihan soal jawab fentrans
Latihan soal jawab fentransWidia Kurnia Adi
 
Latihan soal jawab fentrans
Latihan soal jawab fentransLatihan soal jawab fentrans
Latihan soal jawab fentransWidia Kurnia Adi
 
Chapter16 giancoli edisi 5 jawaban
Chapter16 giancoli edisi 5 jawabanChapter16 giancoli edisi 5 jawaban
Chapter16 giancoli edisi 5 jawabanrisyanti ALENTA
 
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 10 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 10 SolutionsCH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 10 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 10 Solutionssemihypocrite
 
Field exams mxq proplems engineering with solution
Field exams mxq proplems engineering with solutionField exams mxq proplems engineering with solution
Field exams mxq proplems engineering with solutionBaaselMedhat
 
Ap physics b_-_electric_fields_and_forces
Ap physics b_-_electric_fields_and_forcesAp physics b_-_electric_fields_and_forces
Ap physics b_-_electric_fields_and_forcesArvenz Gavino
 

Similar to Anschp23 (15)

Problemas (13 Pág. - 37 Probl.) de Carga Eléctrica y Ley de Coulomb Tippens
Problemas (13 Pág. - 37 Probl.) de Carga Eléctrica y Ley de Coulomb   TippensProblemas (13 Pág. - 37 Probl.) de Carga Eléctrica y Ley de Coulomb   Tippens
Problemas (13 Pág. - 37 Probl.) de Carga Eléctrica y Ley de Coulomb Tippens
 
Problemas (16 Págs. - 42 Probl.) del Capítulo II de Física II
Problemas (16 Págs. - 42 Probl.) del Capítulo II de Física IIProblemas (16 Págs. - 42 Probl.) del Capítulo II de Física II
Problemas (16 Págs. - 42 Probl.) del Capítulo II de Física II
 
Tutorial solutions 2010
Tutorial solutions 2010Tutorial solutions 2010
Tutorial solutions 2010
 
626 pages
626 pages626 pages
626 pages
 
Latihan soal jawab fentrans
Latihan soal jawab fentransLatihan soal jawab fentrans
Latihan soal jawab fentrans
 
Latihan soal jawab fentrans
Latihan soal jawab fentransLatihan soal jawab fentrans
Latihan soal jawab fentrans
 
Chapter16 giancoli edisi 5 jawaban
Chapter16 giancoli edisi 5 jawabanChapter16 giancoli edisi 5 jawaban
Chapter16 giancoli edisi 5 jawaban
 
Magnetism
MagnetismMagnetism
Magnetism
 
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 10 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 10 SolutionsCH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 10 Solutions
CH EN 3453 Heat Transfer 2014 Fall Utah Homework HW 10 Solutions
 
Field exams mxq proplems engineering with solution
Field exams mxq proplems engineering with solutionField exams mxq proplems engineering with solution
Field exams mxq proplems engineering with solution
 
Base excitation of dynamic systems
Base excitation of dynamic systemsBase excitation of dynamic systems
Base excitation of dynamic systems
 
662 magnetrons
662 magnetrons662 magnetrons
662 magnetrons
 
Ap physics b_-_electric_fields_and_forces
Ap physics b_-_electric_fields_and_forcesAp physics b_-_electric_fields_and_forces
Ap physics b_-_electric_fields_and_forces
 
Sm8 21
Sm8 21Sm8 21
Sm8 21
 
Capítulo 11 (5th edition)rewrweerww
Capítulo 11 (5th edition)rewrweerwwCapítulo 11 (5th edition)rewrweerww
Capítulo 11 (5th edition)rewrweerww
 

Anschp23

  • 1. Chapter 23. The Electric Force Physics, 6th Edition Chapter 23. The Electric Force Coulomb's Law 23-1. Two balls each having a charge of 3 ¤ C are separated by 20 mm. What is the force of repulsion between them? (9 x 109 N ⋅ m 2 /C2 )(3 x 10-6 C)(3 x 10-6 C) F= ; F = 202 N (20 x 10-3m) 2 23-2. Two point charges of -3 and +4 o C are 12 mm apart in a vacuum. What is the electrostatic force between them? (9 x 109 N ⋅ m 2 /C2 )(−3 x 10-6 C)(4 x 10-6 C) F= ; F = 750 N, attraction (12 x 10-3 m) 2 23-3. An alpha particle consists of two protons (qe = 1.6 x 10-19 C) and two neutrons (no charge). What is the repulsive force between two alpha particles separated by 2 nm? qα = 2(1.6 x 10-19 C) = 3.2 x 10-19 C (9 x 109 N ⋅ m 2 /C2 )(3.2 x 10-19 C)(3.2 x 10-19 C) F= ; F = 2.30 x 10-10 N (2.00 x 10-9 m) 2 23-4. Assume that the radius of the electron's orbit around the proton in a hydrogen atom is approximately 5.2 x 10-11 m. What is the electrostatic force of attraction? (9 x 109 N ⋅ m 2 /C2 )(1.6 x 10-19 C)(−1.6 x 10-19 C) F= ; F = 8.52 x 10-8 N (5.2 x 10-11m)2 23-5. What is the separation of two -4 a C charges if the force of repulsion between them is 200 N? kqq ' (9 x 109 N ⋅ m 2 /C2 )(−4 x 10-6 C) 2 r= = ; r = 26.8 mm F 200 N 60
  • 2. Chapter 23. The Electric Force Physics, 6th Edition 23-6. Two identical charges separated by 30 mm experience a repulsive force of 980 N. What is the magnitude of each charge? kq 2 Fr 2 (980 N)(0.030 m) 2 F= ; q= = ; q = 9.90 C r2 k 9 x 109 N ⋅ m 2 /C 2 *23-7. A 10 C charge and a -6 r C charge are separated by 40 mm. What is the force between them. The spheres are placed in contact for a few moments and then separated again by 40 mm. What is the new force? Is it attractive or repulsive? (9 x 109 N ⋅ m 2 /C2 )(−6 x 10-6 C)(10 x 10-6 C) F= ; F = 338 N, attraction (40 x 10-3 m) 2 -6 µC 10 µC When spheres touch, 6 e C of charge are neutralized, 0.08 m leaving 4 a C to be shared by two spheres, or 2 µC 2 µC +2 2 C on each sphere. Now they are again separated. 2 µC 2 µC (9 x 109 N ⋅ m 2 /C2 )(2 x 10-6 C)(2 x 10-6 C) F= ; 0.08 m (0.080 m) 2 F = 5.62 N, repulsion *23-8. Two point charges initially attract each other with a force of 600 N. If their separation is reduced to one-third of its original distance, what is the new force of attraction? 2 1  r2  r  F∝ 2; Fr = F r ; 1 1 2 2 2 2 F2 = F1  12  = F1  1  ; r1 = 3 r2 r  r2   r2  2  3r  F2 = F1  2  = 9 F1 ; F2 = 5400 N  r2  61
  • 3. Chapter 23. The Electric Force Physics, 6th Edition The Resultant Electrostatic Force 23-9. A +60 2 C charge is placed 60 mm to the left of a +20 C charge. What is the resultant force on a -35 a C charge placed midway between the two charges? 60 mm (9 x 109 N ⋅ m 2 /C2 )(60 x 10-6 C)(35 x 10-6 C) F13 = +60 µC -35 µC +20 µC (30 x 10-3 m) 2 q1 q3 q2 F13 = 2.10 x 104 N, directed to the left F1 F2 (9 x 10 N ⋅ m /C )(20 x 10 C)(35 x 10 C) 9 2 2 -6 -6 F23 = ; F13 = 2.10 x 104 N, directed to right. (30 x 10-3 m) 2 FR = F13 + F23 = (-2.10 x 104 N) + (0.700 x 104 N); FR = -1.40 x 104 N, left. 23-10. A point charge of +36 2 C is placed 80 mm to the left of a second point charge of -22 C. What force is exerted on third charge of +10 c C located at the midpoint? (9 x 109 N ⋅ m 2 /C2 )(36 x 10-6 C)(10 x 10-6 C) 80 mm F13 = +36 µC 10 µC -22 µC (40 x 10-3 m) 2 q1 q3 F1 q2 F13 = 2025 N, directed to the right F2 (9 x 10 N ⋅ m /C )(22 x 10 C)(10 x 10 C) 9 2 2 -6 -6 F23 = ; F13 = 1238 N, directed to right. (40 x 10-3 m) 2 FR = F13 + F23 = 2025 N + 1238 N; FR = 3260 N, left. 23-11. For Problem 23-10, what is the resultant force on a third charge of +12 2 C placed between the other charges and located 60 mm from the +36 C charge? (9 x 109 N ⋅ m 2 /C2 )(36 x 10-6 C)(12 x 10-6 C 80 mm F13 = +36 µC q3 = 12 µC -22 µC (60 x 10-3 m) 2 60 mm q2 q1 F1 (9 x 109 N ⋅ m 2 /C2 )(22 x 10-6 C)(12 x 10-6 C) F23 = ; F2 (20 x 10-3 m) 2 Both to right, so FR = F13 + F23 = 1080 N + 5940 N; F = 7020 N, rightward. 62
  • 4. Chapter 23. The Electric Force Physics, 6th Edition 23-12. A +6 2 C charge is 44 mm to the right of a -8 € C charge. What is the resultant force on a -2 a C charge that is 20 mm to the right of the -8 C charge? (9 x 109 N ⋅ m 2 /C2 )(8 x 10-6 C)(2 x 10-6 C) 44 mm F13 = -8 µC 24 mm 6 µC q3 = -2 µC (20 x 10-3 m) 2 q2 q1 20 mm F1 (9 x 109 N ⋅ m 2 /C2 )(2 x 10-6 C)(6 x 10-6 C) F2 F23 = ; (24 x 10-3 m) 2 Both to right, so FR = F13 + F23 = 360 N + 187.5 N; F = 548 N, rightward *23-13. A 64-* C charge is locate 30 cm to the left of a 16-h force on a -12 c C charge positioned exactly 50 mm below the 16 s s = (30 mm) 2 + (50 mm) 2 = 58.3 mm +64 µC 30 mm q2 16 µC q1 50 mm φ tan φ = ; φ = 59.0 0 30 mm s (9 x 10 N ⋅ m /C )(64 x 10 C)(12 x 10 C) 9 2 2 -6 -6 50 mm F13 = (58.3 x 10-3 m) 2 F1 F2 F13 = 2033 N, 59.00 N of W φ q3 = -12 µC (9 x 109 N ⋅ m 2 /C2 )(16 x 10-6 C)(12 x 10-6 C) F23 = = 691 N, upward. (50 x 10-3m) 2 Fx = 0 – F13 cos 59.00 = -(2033 N) cos 590 ; Fx = -1047 N Fy = F23 + F13 sin 59.00 = 691 N + (2033 N) sin 590; Fy = 2434 N 2434 N F = ( −1047 N) 2 + (2434 N) 2 = 2650 N; tanθ = ; N = 66.70 N of W. -1047 N Resultant force: FR = 2650 N, 66.70 N of W (or 113.30) 63
  • 5. Chapter 23. The Electric Force Physics, 6th Edition *23-14. A charge of +60 nC is located 80 mm above a -40-nC charge. What is the resultant force on a -50-nC charge located 45 mm horizontally to the right of the -40-nC charge? +60 µC s = (45 mm) 2 + (80 mm) 2 = 91.8 mm q1 80 mm tan φ = ; φ = 60.640 45 mm s 80 mm (9 x 109 N ⋅ m 2 /C2 )(60 x 10-6 C)(50 x 10-6 C) F13 = F1 (91.8 x 10-3 m) 2 F2 q2 F2 F13 = 2564 N, 60.640 N of W 45 mm -40 µC q3 = -50 µC (9 x 109 N ⋅ m 2 /C2 )(40 x 10-6 C)(50 x 10-6 C) F23 = = 8889 N, rightward. (45 x 10-3 m) 2 Fx = – F13 cos 60.640 + F23 = - (2564 N) cos 60.640 + 8889 N ; Fx = 7632 N Fy = +F13 sin 60.640 + 0 = (2564 N) sin 60.640 ; Fy = 2235 N 2235 N F = (7632 N) 2 + (2235 N) 2 ; tanθ = ; FR = 7950 N, 2 = 16.30 N of E. 7632 N *23-15. Three point charges q1 = + 8 C, q2 = -4 C, and q3 = +2 C are placed at the corners of an equilateral triangle, 80 mm on each side as described by Fig. 23-15. What are the magnitude and direction of the resultant force on the +8 e C charge? F2 (9 x 109 N ⋅ m 2 /C 2 )(4 x 10-6 C)(8 x 10-6 C) q1= 8 µC F21 = 600 (80 x 10-3 m) 2 600 80 mm 80 mm F21 = 45.0 N, 600 S of E F1 q3 φ (9 x 109 N ⋅ m 2 /C 2 )(2 x 10-6 C)(8 x 10-6 C) F31 = 80 mm q = -4 µC (80 x 10-3m) 2 +2 µC 2 F31 = 22.5 N, 600 N of E; Fx = (22.5 N) cos 600 + (45 N) cos 600 = 33.8 N Fy = (22.5 N) sin 600 - (45 N) sin 600 = -19.5 N 64
  • 6. Chapter 23. The Electric Force Physics, 6th Edition -19.5 N *23-15. (Cont.) F = (33.8 N) 2 + (−19.5 N) 2 = 39.0 N; tanθ = ; θ = −300 33.8 N Resultant electric force: FR = 39.0 N, e = 330.00 Challenge Problems 23-16. What should be the separation of two +5-uC charges so that the force of repulsion is 4 N? kqq ' (9 x 109 N ⋅ m 2 /C2 )(5 x 10-6 C) 2 r= = ; r = 23.7 cm F 4.00 N 23-17. The repulsive force between two pith balls is found to be 60 h N. If each pith ball carries a charge of 8 nC, what is their separation? kqq ' (9 x 109 N ⋅ m 2 /C2 )(8 x 10-9 C) 2 r= = ; r = 98.0 mm F 60 x 10-6 N 23-18. Two identical unknown charges experience a mutual repulsive force of 48 N when separated by 60 mm. What is the magnitude of each charge? kq 2 Fr 2 (48 N)(0.060 m) 2 F= ; q= = ; q = 4.38 C r2 k 9 x 109 N ⋅ m 2 /C 2 23-19. One object contains an excess of 5 x 1014 electrons and another has a deficiency of 4 x 1014 electrons. What is the force each exerts on the other if the objects are 30 mm apart? Is it attraction or repulsion? ( 1e = 1.6 x 10-19 C, excess = -, deficiency = +. ) q1 = (5 x 1014 e)(1.6 x 10-19 C/e) = -80 1 C; q2 = (4 x 1014 e)(1.6 x 10-19 C/e) = +64 1 C (9 x 109 N ⋅ m 2 /C2 )(80 x 10-6 C)(64 x 10-6 C) F= ; F = 5.12 x 104 N, attraction (30 x 10-3 m) 2 65
  • 7. Chapter 23. The Electric Force Physics, 6th Edition 23-20. If it were possible to put 1 C of charge on each of two spheres separated by a distance of 1 m, what would be the repulsive force in newtons. (9 x 109 N ⋅ m 2 /C2 )(1 C)(1 C) F= ; F = 9 x 109 N ! (1 m) 2 The coulomb is a very large unit for electrostatics applications. 23-21. How many electrons must be placed on each of two spheres separated by 4 mm in order to produce a repulsive force of one 400 N? kq 2 Fr 2 (400 N)(0.004 m) 2 F= ; q= = ; q = 843 nC r2 k 9 x 109 N ⋅ m 2 /C 2  1e  q = 843 x 10-9 C  -19 ; q = 5.27 x 1012 electrons  1.6 x 10 C  23-22. A –40-nC charge is placed 40 mm to the left of a +6-nC charge. What is the resultant force on a –12-nC charge place 8 mm to the right of the +6-nC charge? q3 = -12 nC (9 x 109 N ⋅ m 2 /C2 )(40 x 10-9 C)(12 x 10-9 C) 6 nC F1 = -40 nC 8 mm (48 x 10-3 m) 2 40 mm q1 q2 (9 x 109 N ⋅ m 2 /C2 )(6 x 10-9 C)(12 x 10-9 C) F1 F2 = ; F2 (8 x 10-3 m) 2 Both to right, so FR = F1 + F2 = 1.88 mN – 10.1 mN; F = -8.25 mN, leftward 23-23. A 5-2 C charge is placed 6 cm to the right of a 2-g C charge. What is the resultant force on a –9 nC charge placed 2 cm to the left of the 2-r C charge? (9 x 109 N ⋅ m 2 /C2 )(9 x 10-9 C)(2 x 10-6 C) -9 nC 2 µC 5 µC F1 = 6 cm (2 x 10-2 m) 2 2 cm q1 q2 F1 = +405 mN, to right F1 F2 66
  • 8. Chapter 23. The Electric Force Physics, 6th Edition (9 x 109 N ⋅ m 2 /C2 )(5 x 10-6 C)(9 x 10-9 C) F2 = ; F2 = +63.3 mN, to right (8 x 10-2 m) 2 Resultant force: FR = 405 mN + 63.3 mN; FR = 468 mN 23-24. An equal number of electrons is placed on two metal spheres 3.0 cm apart in air. How many electrons are on each sphere if the resultant force is 4500 N? kq 2 Fr 2 (4500 N)(0.03 m) 2 F= 2 ; q= = ; q = 21.2 C r k 9 x 109 N ⋅ m 2 /C 2  1e  q = 21.2 x 10-6 C  -19 ; q = 1.33 x 1014 electrons  1.6 x 10 C  23-25. A 4-nC charge is placed on a 4-g sphere that is free to move. A fixed 10-n C point charge is 4 cm away. What is the initial acceleration of the 4-o C charge? (9 x 109 N ⋅ m 2 /C2 )(4 x 10-9 C)(10 x 10-6 C) F2 = ; F2 = 225 mN (4 x 10-2 m) 2 F 0.225 N a= = a = 56.2 m/s2 m 0.004 kg *23-26. What is the resultant force on a +2 * C charge an equal distance of 60 mm from each of two –4-g C charges that are 80 mm apart in air? q1= 2 µC 40 mm φ tan φ = ; φ = 48.20 F1 F2 60 mm 60 mm 60 mm (9 x 109 N ⋅ m 2 /C2 )(4 x 10-6 C)(2 x 10-6 C) q3 φ F2 = (60 x 10-3 m) 2 -4 µC q2 = -4 µC F2 = 20.0 N, 48.20 S of E 40 mm (9 x 109 N ⋅ m 2 /C2 )(2 x 10-6 C)(4 x 10-6 C) F1 = ; F1 = 20.0 N, 48.20 S of W (60 x 10-3 m) 2 67
  • 9. Chapter 23. The Electric Force Physics, 6th Edition *23-26. (Cont.) Fx = (20 N) cos 48.20 + (20 N) cos 48.20 = 13.33 N - 13.33 N; Fx = 0 Fy = (20 N) sin 48.20 + (20 N) sin 48.20 = 14.9 N + 14.9 N; Fy = -29.8 N Resultant force: FR = 29.8 N, downward *23-27. Two charges of +25 and +16 * C are 80 mm apart. A third charge of +60 á C is placed between the other charges 30 mm from the +25 i C charge. Find the resultant force on the third charge? 80 mm (9 x 10 N ⋅ m /C )(60 x 10 C)(25 x 10 C) 9 2 2 -6 -6 25 µC q3 = 60 µC 16 µC F1 = (30 x 10-3 m) 2 q2 q1 30 mm 50 mm F2 F1 F1 = 15 kN, directed to the right (9 x 109 N ⋅ m 2 /C2 )(60 x 10-6 C)(16 x 10-6 C) F2 = ; F13 = 3.46 kN, directed to left. (50 x 10-3 m) 2 FR = F1 + F2 = 15 kN + 3.46 kN); FR = 11.5 kN, right. *23-28. A 0.02-g pith ball is suspended freely. The ball is given a charge of +20 l C and placed 0.6 m from a charge of +50 (9 x 109 N ⋅ m 2 /C2 )(20 x 10-6 C)(50 x 10-6 C) F= ; F = 25.0 N (0.600 m) 2 F 25.0 N a= = ; a = 1.25 x 106 m/s m 2 x 10-5 kg *23-29. A 4 * C charge is located 6 cm from an 8 w two charges will the resultant force be zero? F1 = F2 8 µC 4 µC kq3q1 kq3 q2 F1 = F2 ; = x 6 cm - x x 2 (6 − x ) 2 q2 q1 q3 68
  • 10. Chapter 23. The Electric Force Physics, 6th Edition q1 q2 q  F1 = F2 ; = ; x 2 =  1  (6 − x) 2 x 2 (6 − x) 2  q2  q1 4 µC Take square root of both sides: x= (6 - x) = (6 - x); x = 0.707(6 - x) q2 8 µC Solving for x, we obtain: x = 2.49 cm from 4-o C charge *23-30. A charge of +8 nC is placed 40 mm to the left of a –14 nC charge. Where should a third charge be placed if it is to experience a zero resultant force? Considering the sign of the charges and F1 = F2 -14 nC 8 nC their magnitudes, the charge must be to the x 40 mm left of the 8 nC charge as shown. q3 q1 q2 kq3 q1 kq3 q2 q1 q2 q  F1 = F2 ; = F1 = F2 ; = ; x 2 =  1  (40 + x ) 2 x 2 (40 + x) 2 x 2 (40 + x ) 2  q2  Take square root of both sides: q1 8 nC x= (40 + x) = (40 + x); x = 0.756(40+ x) q2 14 nC Solving for x, we obtain: x = 124 mm left of 8 nC charge. *23-31. A +16-* C charge is 80 mm to the right of a +9 t C. Where should a third charge be placed so that the resultant force is zero? F1 = F2 9 µC +16 µC kq3q1 kq3 q2 x F1 = F2 ; = 80 mm - x x 2 (80 − x ) 2 q1 q3 q2 q1 q2 q  F1 = F2 ; = ; x 2 =  1  (80 − x ) 2 x 2 (80 − x) 2  q2  q1 9 µC Take square root of both sides: x= (80 - x) = (80 - x); x = 0.750(80 - x) q2 16 µ C 69
  • 11. Chapter 23. The Electric Force Physics, 6th Edition Solving for x, we obtain: x = 34.3 mm from 9-o C charge *23-32. Two 3-g spheres are suspended from a common point with two 80 mm light silk threads of negligible mass. What charge must be placed on each sphere if their final positions are 50 mm apart? T 80 mm 25 mm F φ F cos φ = ; φ = 71.80 Ty = T sin φ = mg 80 mm mg mg mg (3 x 10-3 kg)(9.8 m/s 2 ) 25 mm T= = ; T = 30.9 mN sin φ sin 71.80 Tx = T cos 71.80 = (30.9 mN) cos 71.80; Tx = 9.67 mN; ΣFx = 0: F = Tx kq 2 Fr 2 (9.67 x 10-3 N)(50 x 10-3m) 2 F = 2 = 9.67 mN; q= = ; q = 51.8 nC r k 9 x 109 N ⋅ m 2 /C2 Critical Thinking Questions *23-33. A small metal sphere is given a charge of +40 h C, and a second sphere 8 cm away is given a charge of –12 s C. What is the force of attraction between them? If the two spheres are allowed to touch and are then again placed 8 cm apart, what new electric force exists between them? Is it attraction or repulsion? (9 x 109 N ⋅ m 2 /C2 )(12 x 10-6 C)(40 x 10-6 C) F= ; F = 675 N, attraction (0.080 m) 2 40 µC -12 µC When spheres touch, 6 4 C of charge are neutralized, 0.08 m leaving 28 l C to be shared by two spheres, or 14 µC 14 µC +14 t C on each sphere. Now they are again separated: 14 µC 14 µC 0.08 m (9 x 109 N ⋅ m 2 /C2 )(14 x 10-6 C)(14 x 10-6 C) F= ; (0.080 m) 2 70
  • 12. Chapter 23. The Electric Force Physics, 6th Edition F = 276 N, repulsion *23-34. The total charge on two metal spheres 50 mm apart is 80 * C. If they repel each other with a force of 800 N, what is the charge on each sphere? 50 mm q1 q2 q1 + q2 = 80 q C; q2 = 80 q C – q1 kq1q2 kq1 (80 µ C - q1 ) kq1 (80µ C ) − kq12 Fr 2 F= = ; F= ; = (80 µ C)q1 − q12 r2 r2 r2 k (800 N)(50 x 10-3 m) 2 = (80 µ C)q1 − q12 ; q12 – (80 x 10-6 C)q1+ 222 x 10-12 C2 = 0 (9 x 109 N ⋅ m 2 /C2 ) Solve the quadratic equation with a = 1, b = - 80 x 10-6, and c = 222 x 10-12 q1 = 77.1 0 C and q1 = 2.89 0 C Now q2 = 80 C – q1 yields the following : q2 = 2.89 = C and q2 = 77.1 n C Thus, one charge is 77.1 C and the other is 2.89 i C *23-35. Four small spheres are each given charges of q = +20 * C and placed at the corners of a square with sides of length 6 cm. Show that the resultant force on each charge has a magnitude equal to 1914 N. What is the direction of the force? What will change if the charges are each q = -20 C? (Like charges repel, so sign doesn’t matter.) F1 F2 φ q 6 cm R = (6 cm) + (6 cm) = 8.485 cm 2 2 F1 (9 x 109 N ⋅ m 2 /C2 )(20 x 10-6 C)(20 x 10-6 C) F1 = 6 cm (6 x 10-2 m) 2 R 6 cm (9 x 109 N ⋅ m 2 /C2 )(20 x 10-6 C)(20 x 10-6 C) φ F2 = (8.485 x 10-2 m) 2 q q 6 cm F1 = 1000 N; F2 = 500 N; For a square, the angle φ = 450 Fx = (1000 N) + (500 N) cos 450 + 0 = 1354 N; Fy = 1000 N + (500 N) sin 450 = 1354 N 71
  • 13. Chapter 23. The Electric Force Physics, 6th Edition F = (1354 N) 2 + (1354 N) 2 ; F = 1914 N, 450 away from center. *23-36. Two charges q1 and q2 are separated by a distance r. They experience a force F at this distance. If the initial separation is decreased by only 40 mm, the force between the two charges is doubled. What was the initial separation? F x F 2kq1q2 kq1q2 2 1 q1 q2 = ; = x 2 ( x − 40 mm) 2 x 2 ( x − 40 mm) 2 x – 40 mm 2 2 x = 2(x – 40 mm) Take square root of both sides: q1 2F 2F q2 x = 1.414(x – 40 mm); x = 137 mm *23-37. Two 8-g pith balls are suspended from silk threads 60 cm long and attached to a common point. When the spheres are given equal amounts of negative charge, the balls come to rest 30 cm apart. Calculate the magnitude of the charge on each pith ball. 0.15 m cos φ = ; φ = 75.50 Ty = T sin φ = mg T 0.60 m 0.6 m F φ F -3 2 mg (8 x 10 kg)(9.8 m/s ) T= = ; T = 81.0 mN sin φ sin 75.50 mg mg 0.15 m Tx = T cos 71.80 = (81.0 mN) cos 75.50; Tx = 20.25 mN; ΣFx = 0: F = Tx kq 2 Fr 2 (2.025 x 10-4 N)(0.30 m) 2 F = 2 = 20.25 mN; q= = ; q = -450 nC r k 9 x 109 N ⋅ m 2 /C2 72