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Chapter 15

Chapter 15. Electric Forces and Electric Fields. Unfinished business…. How many electrons? M=357.2g C 12 H 22 O 11. < 10 6 < 10 12 < 10 18 < 10 24 < 10 30 < 10 36 < 10 42. Unfinished business…. How many electrons? m=357.2g C 12 H 22 O 11. < 10 25 < 10 26 < 10 27 < 10 28

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Chapter 15

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  1. Chapter 15 Electric Forces and Electric Fields

  2. Unfinished business… How many electrons? M=357.2g C12H22O11 • < 106 • < 1012 • < 1018 • < 1024 • < 1030 • < 1036 • < 1042

  3. Unfinished business… How many electrons? m=357.2g C12H22O11 • < 1025 • < 1026 • < 1027 • < 1028 • < 1029 • < 1030

  4. Unfinished business… How many electrons? M=357.2g C12H22O11 • < 1x1026 • < 2x1026 • < 3x1026 • < 4x1026 • < 5x1026 • < 6x1026 • < 7x1026 • < 8x1026 • < 9x1026 • < 1.0x1027

  5. Unfinished business… How many electrons? M=357.2g C12H22O11 • < 1.1x1026 • < 1.2x1026 • < 1.3x1026 • < 1.4x1026 • < 1.5x1026 • < 1.6x1026 • < 1.7x1026 • < 1.8x1026 • < 1.9x1026 • < 2.0x1026

  6. Quiz: Which quantity is not always conserved? • Charge • Energy • Mass • Momentum

  7. Review • Electric Charge • Two types: + (proton), - (electron), same magnitude • SI Unit of charge: Coulomb (huge!) 1C = 1A1s • Charge is conserved (but not mass!) • Charge is quantized in multiples of e = 1.6x10-19 C • Methods of charging objects • Friction, Conduction, Induction, Polarization, Grounding • Coulomb’s Law • Opposite charges attract; like charges repel. • Force proportional to both charges • and the inverse square of separation • Comparison with gravity • Superposition principle

  8. Electric Fields Sections 4 – 6

  9. Electrical Field Michael Faraday (1791 – 1867) 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

  10. Action at a Distance • Contact forces • Local: force transmitted by touching • Field forces • Action at a distance – no touching • Eg. Gravity and Electricity • Actually all fundamental forces! • Can think of field as producing a local force • But or course the field is created at a distance

  11. Electric Field, cont. Coulomb’s law is symmetric for the two charges; let’s break it up A charged particle, with charge Q, produces an electric field in the region of space around it A small test charge, qo, placed in the field, will experience a force from the electric field Why must q0 be small? field MU28T11-12: Electric Force Field

  12. Electric Field Definition Mathematically, SI units are N / C 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

  13. Electric Field due to a Positive Spherical or Point Charge 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 The magnitude of the electric field produced by the positive charge is

  14. 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 The magnitude of the electric field produced by the negative charge is Electric Field due to a Negative Spherical or Point Charge Active Figure: The Small Positive Test Charge

  15. 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

  16. Are Electric Fields Real? Why bother with fields instead of just using the force? The only way to measure it is to putting a test charge in the field Then you are back to Coulomb’s law! If a tree falls in the forest, and no one hears it…? However: the concept of field will be extremely useful in understanding later chapters Electric fields can generate magnetic fields and vice versa. (not just created by charge) Electric and Magnetic fields are the medium of light waves(waves are the ripples of E&M fields)

  17. Problem Solving Strategy, Electric Fields Calculate Electric Fields of point charges Use the equation to find the electric field due to the individual charges The direction is given by the direction of the force on a positive test charge The Superposition Principle can be applied if more than one charge is present EX15.5

  18. 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

  19. Electric Field Lines, cont. The field lines are related to the field in the following manners: The electric field vector, , 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 MU28T14: Electric Field Lines

  20. Electric Field Line Patterns Point charge The lines radiate equally in all directions For a positive source charge, the lines will radiate outward For a negative source charge, the lines will point inward

  21. 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

  22. Electric Field Line Patterns Two equal but like point charges 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

  23. Electric Field Patterns Unequal and unlike charges Note that two lines leave the +2q charge for each line that terminates on -q Active Figure: Electric Field Lines

  24. 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

  25. Atmospheric Electric Fields The electric field near the surface of the Earth in fair weather is about 100 N/C downward Under a thundercloud, the electric field can very large, on the order of 20,000 N/C A device for measuring these fields is called the field mill

  26. 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 in electrostatic equilibrium has four important properties

  27. 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

  28. Property 2 Any excess charge on an isolated conductor resides entirely on its surface A direct result of the 1/r2 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

  29. Property 3 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 • The electric field just outside a charged conductor is perpendicular to the conductor’s surface

  30. Quiz: what is the best shape for a lightning rod? • .. • .. • .. • .. 1. 2. 3. 4.

  31. 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) Why a lightning rod works

  32. Experiment to Verify Properties of Charges Faraday’s Ice-Pail Experiment A charged object suspended inside a metal container causes a rearrangement of charge on the container in such a manner that the sign of the charge on the inside surface of the container is opposite the sign of the charge on the suspended object Any charge transferred to a conductor resides on its surface in electrostatic equilibrium

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