CHAPTER 18 ELECTRIC FORCES AND ELECTRIC FIELDS PROBLEMS ______________________________________________________________________________ 7. SSM WWW REASONING Initially, the two spheres are neutral. Since negative charge is removed from the sphere which loses electrons, it then carries a net positive charge. Furthermore, the neutral sphere to which the electrons are added is then negatively charged. Once the charge is transferred, there exists an electrostatic force on each of the two spheres, the magnitude of which is given by Coulomb's law (Equation 18.1), F kq1q2 / r 2 . SOLUTION a. Since each electron carries a charge of –1.60 u 10 –19 C, the amount of negative charge removed from the first sphere is § 1.60 u 1019 C · 3.0 u 1013 electrons ¨ ¸ © 1 electron ¹ 4.8 u 106 C Thus, the first sphere carries a charge +4.8 u 10–6 C, while the second sphere carries a 6 charge –4.8 u10 C . The magnitude of the electrostatic force that acts on each sphere is, therefore, kq 1 q 2 (8.99 u 10 9 N m 2 /C 2 )(4.8 u 10 – 6 C) 2 F 0.83 N r2 (0.50 m) 2 b. Since the spheres carry charges of opposite sign, the force is attractive . ______________________________________________________________________________ 15. SSM WWW REASONING Each particle will experience an electric force due to the presence of the other charge. According to Coulomb's law (Equation 18.1), the magnitude of the force felt by each particle can be calculated from F kq1q2 / r 2 , where q1 and q2 are the respective charges on particles 1 and 2 and r is the distance between them. According to Newton's second law, the magnitude of the force experienced by each particle is given by F ma , where a is the acceleration of the particle. SOLUTION a. Since the two particles have identical positive charges, q1 the data for particle 1, kq 2 m1a1 2 r q2 q , and we have, using 664 ELECTRIC FORCES AND ELECTRIC FIELDS Solving for q, we find that m 1 a1 r 2 q (6.00 u 10 –6 kg) (4.60 u 10 3 m/s 2 ) (2.60 u 10 –2 m) 2 8.99 u 10 9 N m 2 /C 2 k 4.56 u 10 –8 C b. Since each particle experiences a force of the same magnitude (From Newton's third law), we can write F1 F2 , or m1a1 m2 a2 . Solving this expression for the mass m 2 of particle 2, we have (6.00 u 10 –6 kg)(4.60 u 10 3 m/s 2 ) m2 3.25 u 10 –6 kg 3 2 a2 8.50 u 10 m/s ______________________________________________________________________________ m 1 a1 E2 REASONING The 39. SSM WWW figure shows the arrangement of the three charges. Let E q represent the electric field at the empty corner due to the –q charge. Furthermore, let E1 and E2 be the electric fields at the empty corner due to charges +q1 and +q2, respectively. E1 +q1 Eq d 5 T –q d +q2 2d According to the Pythagorean theorem, the distance from the charge –q to the empty corner along the diagonal is given by (2d ) 2 d 2 5d 2 d 5 . The magnitude of each electric field is given by Equation 18.3, E electric fields at the empty Eq kq / r 2 2 kq / d 5 2 kq / r . Thus, the magnitudes of each of the corner are given as follows: 2 kq /(5d ) , since the length of the diagonal is d 5 ; 2 2 E1 kq1 /(4d ) ; and E2 kq2 / d . The angle T that the diagonal makes with the horizontal is T tan 1 (d / 2d) 26.57q . Since the net electric field Enet at the empty corner is zero, the horizontal component of the net field must be zero, and we have E1 – E q cos 26.57q 0 or kq 1 / 4 d 2 – kq cos 26.57q / 5d 2 Similarly, the vertical component of the net field must be zero, and we have E 2 – E q sin 26.57q 0 or kq 2 / d 2 – kq sin 26.57q / 5d 2 0 These last two expressions can be solved for the charges q1 and q2 . SOLUTION Solving the last two expressions for the charges q1 and q2 , we have 0 Chapter 18 Problems q1 4 q 5 cos 26.57q 0.716 q q2 1 q 5 sin 26.57q 0.0895 q 665 ______________________________________________________________________________ 59. SSM WWW REASONING Two forces act on the charged ball (charge q); they are the downward force of gravity mg and the electric force F due to the presence of the charge q in the electric field E. In order for the ball to float, these two forces must be equal in magnitude and opposite in direction, so that the net force on the ball is zero (Newton's second law). Therefore, F must point upward, which we will take as the positive direction. According to Equation 18.2, F = qE. Since the charge q is negative, the electric field E must point downward, as the product qE in the expression F = qE must be positive, since the force F points upward. The magnitudes of the two forces must be equal, so that mg qE . This expression can be solved for E. SOLUTION The magnitude of the electric field E is E mg q (0.012 kg)(9.80 m/s 2 ) 18 u 10 –6 C 6.5 u 10 3 N/C As discussed in the reasoning, this electric field points downward . ______________________________________________________________________________