Electric Fields Required Background Knowledge Section 7.1, pages 320326 Section 7.1 Properties of Electric Charges 1. Law of electric charges, like charges repel and opposites attract 2. Charges are due to an excess or deficit of negative charges (electrons). Protons are positively charged and remain in nucleus 3. Electric charge: the unit of charge (q) is the Coulomb (C) which represents the “charge” on a group of electrons (-) or protons (+). The charge on an electron (qe-) is -1.6 x 10-19C and the charge on a proton (qp+) is +1.6 x 10-19C. So 1 C=6.25 x 1018 electrons or protons. 4. Conductors and Insulators 5. Charging of objects by the transfer of electrons 1 Coulomb’s Law Two similarly charged masses will exert a force of electrostatic repulsion (Fe) on each other. What parameters would affect the magnitude of this force? - amount of charge (q) on each - distance between them (r) The forces can be analyzed by standard FBDs and dynamics. Henri Cavendish studied electrostatic forces with a torsion balance. 2 Deriving Coulomb’s Law Using proportional techniques we can determine: 1 F q1q2 and F 2 r so altogether q1q2 F 2 and then r qq F k 1 22 r Henri Cavendish determined the constant of proportionality (k) to be 9.0 x 109 N·m2/C2 3 Coulomb’s Law Déjà vu - Gravity 4 Coulomb’s law can be used… (a) Comparatively using: F1 q1q2 F2 q1 ' q2 ' where the ' (prime sign) represents either of the two charges being changed to a secondary value. Example: #4, page 333 5 (b) Directly using kq1q2 Fe 2 r What is the electrostatic force exerted between the two charges q1 and q2 as shown? 6 Do not forget the Vector Nature of the electrostatic force. Example: Find the total force on charge q3 in the charge distribution given here. 7 Example: Deals with a practical application of forces on charges (electrons) in a conductor. The mutual repulsion means that electrons actually travel in the outer regions of any conductor. Find the force on any of the three electrons as a result of being forced by the other two. Further questions - Do 1 – 10, page 333 8