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Electric Potential Chapter 26 physics chapter 26 1 Review from ch 7 W12 U1 U 2 When positive work is done, the potential energy decreases. K1 U1 K2 U 2 Total energy is conserved. physics chapter 26 2 Work done by E field Wab Fd qEd Using calculus and the coulomb force equation, we can come up with Wab q1q2 1 1 40 ra rb physics chapter 26 3 Work done by E field We can write using potential energy Wab U a U b Thus 1 q1q2 U 40 r physics chapter 26 4 Example A small plastic ball with a mass of 2.0 g and an electric charge of 0.10 mC moves in the vicinity of a stationary metal ball with a charge of 2.0 mC. When the plastic ball is 0.10 m from the metal one, the plastic ball is moving directly away from the metal one with a speed of 5.0 m/s. What is the speed of the plastic ball when the two balls are 0.20 m apart? physics chapter 26 5 You try What if the plastic ball had a charge of -0.10 mC? physics chapter 26 6 Potential Potential energy per unit charge U V q U qV Measured in volts J 1V 1 C physics chapter 26 7 Potential from a group of charges qi V 40 ri 1 physics chapter 26 8 Example Pages 583-584 physics chapter 26 9 Equipotential surfaces A surface such that every point on the surface has the same potential. Since the potential is the same, E does no work as a charge moves along an equipotential surface. physics chapter 26 10 Millikan oil-drop experiment 1909-1913 in Chicago by Robert Millikan Very small electrically charged oil drops sprayed into electric field Field adjusted until the gravitational force down balanced the electric force up. Figured out charge on the oil drops. physics chapter 26 11 Millikan oil-drop experiment Figured out that the charge was always a whole number multiple of 1.6 x 10-19 “discovered” the charge on the electron Validation of atomic theory Combined with earlier research of J.J. Thomson to determine mass of electron physics chapter 26 12 Mass of oil drops mg q E mgd q V 4 r gd q 3 V 3 3 d vt q 18 V 2 g 3 physics chapter 26 13 Electronvolt Unit of energy (like J) Useful in atomic and nuclear calculations 1 eV = 1.6 x 10-19 J The change in energy as 1 electron moves through a potential difference of 1 V physics chapter 26 14 Rest energy E0 = mc2 For an electron, 81.87 x 10-15 J or 0.511 MeV Mass of subatomic particles is often expressed in MeV/c2 to make the numbers easier to work with Mass of electron = 0.511 MeV/c2 physics chapter 26 15 Cathode ray tubes Found in computer monitors and oscilloscopes Similar to TV picture tubes Use an electron beam – historically called a cathode ray A near vacuum Electrons sent through two sets of electrically charged plates One to aim it horizontally One to aim it vertically physics chapter 26 16 Equations We did this kind of problem last chapter There are more equations on pages 594 595 physics chapter 26 17