Chapter 17 & 18. Electric Field and Electric Potential

Transcription

1 Chapter 17 & 18 Electric Field and Electric Potential

2 Electric Field Maxwell developed an approach to discussing fields An electric field is said to exist in the region of space around a charged object When another charged object enters this electric field, the field exerts a force on the second charged object

3 Electric Field, cont. A charged particle, with charge Q, produces an electric field in the region of space around it A small test charge, q o, placed in the field, will experience a force

4 Electric Field Mathematically, F E = = q Use this for the magnitude of the field The electric field is a vector quantity The direction of the field is defined to be the direction of the electric force that would be exerted on a small positive test charge placed at that point o k eq 2 r

5 Direction of Electric Field The electric field produced by a negative charge is directed toward the charge A positive test charge would be attracted to the negative source charge

6 Direction of Electric Field, cont The electric field produced by a positive charge is directed away from the charge A positive test charge would be repelled from the positive source charge

7 More About a Test Charge and The Electric Field The test charge is required to be a small charge It can cause no rearrangement of the charges on the source charge The electric field exists whether or not there is a test charge present The Superposition Principle can be applied to the electric field if a group of charges is present

8 Problem Solving Strategy Units When using k e, charges must be in Coulombs, distances in meters and force in Newtons If values are given in other units, they must be converted Applying Coulomb s Law to point charges Use the superposition principle for more than two charges Use Coulomb s Law to find the individual forces Directions of forces are found by noting that like charges repel and unlike charges attract

9 Electric Field Lines A convenient aid for visualizing electric field patterns is to draw lines pointing in the direction of the field vector at any point These are called electric field lines and were introduced by Michael Faraday

10 Electric Field Lines, cont. The field lines are related to the field by The electric field vector, E, is tangent to the electric field lines at each point The number of lines per unit area through a surface perpendicular to the lines is proportional to the strength of the electric field in a given region

11 Electric Field Line Patterns Point charge The lines radiate equally in all directions For a positive source charge, the lines will radiate outward

12 Electric Field Line Patterns For a negative source charge, the lines will point inward

13 Electric Field Line Patterns An electric dipole consists of two equal and opposite charges The high density of lines between the charges indicates the strong electric field in this region

14 Electric Field Line Patterns Two equal but like point charges At a great distance from the charges, the field would be approximately that of a single charge of 2q The bulging out of the field lines between the charges indicates the repulsion between the charges The low field lines between the charges indicates a weak field in this region

15 Electric Field Patterns Unequal and unlike charges Note that two lines leave the +2q charge for each line that terminates on -q

16 Rules for Drawing Electric Field Lines The lines for a group of charges must begin on positive charges and end on negative charges In the case of an excess of charge, some lines will begin or end infinitely far away The number of lines drawn leaving a positive charge or ending on a negative charge is proportional to the magnitude of the charge No two field lines can cross each other

17 Conductors in Electrostatic Equilibrium When no net motion of charge occurs within a conductor, the conductor is said to be in electrostatic equilibrium An isolated conductor has the following properties: The electric field is zero everywhere inside the conducting material Any excess charge on an isolated conductor resides entirely on its surface The electric field just outside a charged conductor is perpendicular to the conductor s surface On an irregularly shaped conductor, the charge accumulates at locations where the radius of curvature of the surface is smallest (that is, at sharp points)

18 Property 1 The electric field is zero everywhere inside the conducting material Consider if this were not true if there were an electric field inside the conductor, the free charge there would move and there would be a flow of charge If there were a movement of charge, the conductor would not be in equilibrium

19 Property 2 Any excess charge on an isolated conductor resides entirely on its surface A direct result of the 1/r 2 repulsion between like charges in Coulomb s Law If some excess of charge could be placed inside the conductor, the repulsive forces would push them as far apart as possible, causing them to migrate to the surface

20 Property 3 The electric field just outside a charged conductor is perpendicular to the conductor s surface Consider what would happen it this was not true The component along the surface would cause the charge to move It would not be in equilibrium

21 Property 4 On an irregularly shaped conductor, the charge accumulates at locations where the radius of curvature of the surface is smallest (that is, at sharp points)

22 Property 4, cont. Any excess charge moves to its surface The charges move apart until an equilibrium is achieved The amount of charge per unit area is greater at the flat end The forces from the charges at the sharp end produce a larger resultant force away from the surface Why a lightning rod works

23 Electric Field of a Charged Thin Spherical Shell The calculation of the field outside the shell is identical to that of a point charge Q E = = 2 4πr ε o k e Q 2 r The electric field inside the shell is zero

24 Electric Field of a Nonconducting Plane Sheet of Charge Use a cylindrical Gaussian surface The flux through the ends is EA, there is no field through the curved part of the surface The total charge is Q = σa E = σ 2ε Note, the field is uniform o

25 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

26 Work and Potential Energy There is a uniform field between the two plates As the charge moves from A to B, work is done in it W = F d= q E d ΔPE = - W = - q E d only for a uniform field

27 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 ΔV V = V B V A = ΔPE / q Potential difference is not the same as potential energy

28 Potential Difference, cont. Another way to relate the energy and the potential difference: ΔPE = q ΔV 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 B V A = -Ed Gives more information about units: N/C = V/m

29 Energy and Charge Movements 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

30 Energy and Charge Movements, cont 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 potential energy

31 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

32 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 decreases Its kinetic energy increases

33 Electric Potential of a Point Charge 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 V = k e q r A potential exists at some point in space whether or not there is a test charge at that point

34 Electric Potential of Multiple Point Charges 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 The algebraic sum is used because potentials are scalar quantities

35 Electrical Potential Energy of Two Charges V 1 is the electric potential due to q 1 at some point P 1 The work required to bring q 2 from infinity to P 1 without acceleration is q 2 V 1 This work is equal to the potential energy of the two particle system q1q 2 PE = q2 V1 = ke r

36 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 The force would be attractive Work must be done to hold back the unlike charges from accelerating as they are brought close together

37 Problem Solving with Electric Potential (Point Charges) Remember that potential is a scalar quantity So no components to worry about Use the superposition principle when you have multiple charges Take the algebraic sum Keep track of sign The potential is positive if the charge is positive and negative if the charge is negative Use the basic equation V = k e q/r