8/31/2011 Question I Chapter 16 Electric Energy and Capacitance Three equal positive charges are placed on the x-axis, one at the origin, one at x = 2 m, and the third at x = 4 m. Of the following points, which has the greatest magnitude electric field? a. x = 1 m b. x = 3 m c. x = 5 m e. The electric field has the same magnitude at all three positions. Ea = -1/9, Question II Summary If the distance between two equal point charges is tripled, and the charges are doubled, the mutual force between them will be changed by what factor? a. 9.0 b. 3.0 c. 4.33 d. 4/9 e. 4 Electric Potential Energy The electrostatic force is a conservative force It is possible to define an electrical potential energy function with this force Work done by a conservative force is equal to the negative of the change in potential energy Eb = 1/9, Ec = 1.15 in units of kQ Potential and Potential difference Potential due to point charges Energy conservation Work and Potential Energy There is a uniform field between the two plates As the charge moves from A to B, work is done on it W = Fd=q Ex (xf – xi) ∆PE = - W = - q Ex ∆x Only for a uniform field 1 8/31/2011 Potential Difference The potential difference between points A and B is defined as the change in the potential energy (final value minus initial value) of a charge q moved from A to B divided by the size of the charge Potential Difference, cont. ∆V = VB – VA = ∆PE / q Potential difference is not the same as potential energy Another way to relate the energy and the potential difference: ∆PE = q ∆V Both electric potential energy and potential difference are scalar quantities Units of potential difference V = J/C A special case occurs when there is a uniform electric field ∆V = VB – VA= -Ex ∆x Potential Energy Compared to Potential Electric potential is characteristic of the field only Independent of any test charge that may be placed in the field Due to an interaction between the field and the charge placed in the field Energy and Charge Movements, cont Energy and Charge Movements Electric potential energy is characteristic of the charge-field system When the electric field is directed downward, point B is at a lower potential than point A A positive test charge that moves from A to B loses electric potential energy It will gain the same amount of kinetic energy as it loses in potential energy Gives more information about units: N/C = V/m A positive charge gains electrical potential energy when it is moved in a direction opposite the electric field If a charge is released in the electric field, it experiences a force and accelerates, gaining kinetic energy As it gains kinetic energy, it loses an equal amount of electrical potential energy A negative charge loses electrical potential energy when it moves in the direction opposite the electric field Summary of Positive Charge Movements and Energy When a positive charge is placed in an electric field It moves in the direction of the field It moves from a point of higher potential to a point of lower potential Its electrical potential energy decreases Its kinetic energy increases 2 8/31/2011 Electric Potential of a Point Charge Summary of Negative Charge Movements and Energy When a negative charge is placed in an electric field It moves opposite to the direction of the field It moves from a point of lower potential to a point of higher potential Its electrical potential energy increases Its kinetic energy increases Work has to be done on the charge for it to move from point A to point B V = ke The electric field is proportional to 1/r2 The electric potential is proportional to 1/r A potential exists at some point in space whether or not there is a test charge at that point Superposition principle applies The total electric potential at some point P due to several point charges is the algebraic sum of the electric potentials due to the individual charges Potential is plotted on the vertical axis In arbitrary units Two charges have equal magnitudes and opposite charges Example of superposition The algebraic sum is used because potentials are scalar quantities Electrical Potential Energy of Two Charges Dipole Example q r Electric Potential of Multiple Point Charges Electric Field and Electric Potential Depend on Distance The point of zero electric potential is taken to be at an infinite distance from the charge The potential created by a point charge q at any distance r from the charge is V1 is the electric potential due to q1 at some point P The work required to bring q2 from infinity to P without acceleration is q2V1 This work is equal to the potential energy of the two particle system PE = q2 V1 = k e q1q2 r 3 8/31/2011 Notes About Electric Potential Energy of Two Charges If the charges have the same sign, PE is positive Positive work must be done to force the two charges near one another The like charges would repel If the charges have opposite signs, PE is negative Draw a diagram of all charges Note the point of interest Calculate the distance from each charge to the point of interest Use the basic equation V = keq/r Include the sign The potential is positive if the charge is positive and negative if the charge is negative 16.13 Electric potential at NE corner Use the superposition principle when you have multiple charges The force would be attractive Work must be done to hold back the unlike charges from accelerating as they are brought close together Problem Solving with Electric Potential, cont Problem Solving with Electric Potential (Point Charges) Take the algebraic sum Remember that potential is a scalar quantity So no components to worry about Problem 16.23 α particles charge 2e and mass 4 mp and moving at 2 x 107 m/s. How close do they get to a gold nucleus (79e). Summary Potential and Potential difference Potential due to point charges Energy conservation Charged conductors Equipotential surfaces Topography of energy landscapes 4