Lecture Outline Chapter 16 College Physics 7 th

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Lecture Outline Chapter 16 College Physics, 7 th Edition Wilson / Buffa / Lou

Lecture Outline Chapter 16 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.

Chapter 16 Electric Potential, Energy, and NO – Capacitance © 2010 Pearson Education, Inc.

Chapter 16 Electric Potential, Energy, and NO – Capacitance © 2010 Pearson Education, Inc.

Units of Chapter 16 Electric Potential Energy and Electric Potential Difference Equipotential Surfaces and

Units of Chapter 16 Electric Potential Energy and Electric Potential Difference Equipotential Surfaces and the Electric Field Capacitance Dielectrics Capacitors in Series and in Parallel © 2010 Pearson Education, Inc.

16. 1 Electric Potential Energy and Electric Potential Difference It takes work to move

16. 1 Electric Potential Energy and Electric Potential Difference It takes work to move a charge against an electric field. Just as with gravity, this work increases the potential energy of the charge. © 2010 Pearson Education, Inc.

16. 1 Electric Potential Energy and Electric Potential Difference Just as with the electric

16. 1 Electric Potential Energy and Electric Potential Difference Just as with the electric field, it is convenient to define a quantity that is the electric potential energy per unit charge. This is called the electric potential. Unit of electric potential: the volt, V © 2010 Pearson Education, Inc.

16. 1 Electric Potential Energy and Electric Potential Difference The potential difference between parallel

16. 1 Electric Potential Energy and Electric Potential Difference The potential difference between parallel plates can be calculated relatively easily: For a pair of oppositely charged parallel plates, the positively charged plate is at a higher electric potential than the negatively charged one by an amount ΔV. © 2010 Pearson Education, Inc.

16. 1 Electric Potential Energy and Electric Potential Difference As with potential energy, only

16. 1 Electric Potential Energy and Electric Potential Difference As with potential energy, only changes in the electric potential can be defined. The choice of V = 0 is arbitrary. © 2010 Pearson Education, Inc.

16. 1 Electric Potential Energy and Electric Potential Difference Electric potential difference of a

16. 1 Electric Potential Energy and Electric Potential Difference Electric potential difference of a point charge – just like energy, not path dependent: © 2010 Pearson Education, Inc.

16. 1 Electric Potential Energy and Electric Potential Difference Whether the electric potential increases

16. 1 Electric Potential Energy and Electric Potential Difference Whether the electric potential increases or decreases when towards or away from a point charge depends on the sign of the charge. Electric potential increases when moving nearer to positive charges or farther from negative charges. Electric potential decreases when moving farther from positive charges or nearer to negative charges. © 2010 Pearson Education, Inc.

16. 1 Electric Potential Energy and Electric Potential Difference The electric potential energy of

16. 1 Electric Potential Energy and Electric Potential Difference The electric potential energy of two charges is the change in electric potential multiplied by the charge. © 2010 Pearson Education, Inc.

16. 1 Electric Potential Energy and Electric Potential Difference The additional potential energy due

16. 1 Electric Potential Energy and Electric Potential Difference The additional potential energy due to a third charge is the sum of its potential energies relative to the first two. Further charges extend the sum. © 2010 Pearson Education, Inc.

16. 2 Equipotential Surfaces and the Electric Field An equipotential surface is one on

16. 2 Equipotential Surfaces and the Electric Field An equipotential surface is one on which the electric potential does not vary; it takes no work to move a charge along an equipotential surface. © 2010 Pearson Education, Inc.

16. 2 Equipotential Surfaces and the Electric Field Equipotentials are analogous to contour lines

16. 2 Equipotential Surfaces and the Electric Field Equipotentials are analogous to contour lines on a topographic map. © 2010 Pearson Education, Inc.

16. 2 Equipotential Surfaces and the Electric Field Equipotentials are always perpendicular to electric

16. 2 Equipotential Surfaces and the Electric Field Equipotentials are always perpendicular to electric field lines. This enables you to draw one if you know the other. © 2010 Pearson Education, Inc.

16. 2 Equipotential Surfaces and the Electric Field Here, these principles have been used

16. 2 Equipotential Surfaces and the Electric Field Here, these principles have been used to draw the electric field lines and equipotentials of an electric dipole. © 2010 Pearson Education, Inc

16. 2 Equipotential Surfaces and the Electric Field © 2010 Pearson Education, Inc.

16. 2 Equipotential Surfaces and the Electric Field © 2010 Pearson Education, Inc.

16. 2 Equipotential Surfaces and the Electric Field The electron-volt (e. V) is the

16. 2 Equipotential Surfaces and the Electric Field The electron-volt (e. V) is the amount of energy needed to move an electron through a potential difference of one volt. The electron-volt is a unit of energy, not voltage, and is not an SI standard unit. It is, however, quite useful when dealing with energies on the atomic scale. © 2010 Pearson Education, Inc.

Review of Chapter 16 Electric potential difference between two points is the work done

Review of Chapter 16 Electric potential difference between two points is the work done per unit charge in moving a charge between those two points. Equipotential surfaces are surfaces on which the electric potential is constant. Electric potential for a point charge: Electric potential energy for a pair of point charges: © 2010 Pearson Education, Inc.

Review of Chapter 16 Electric potential energy for an array of point charges: The

Review of Chapter 16 Electric potential energy for an array of point charges: The electric field is in the direction of maximum change of the electron potential. Magnitude: © 2010 Pearson Education, Inc.

Review of Chapter 16 An electron-volt is the energy gained by an electron accelerating

Review of Chapter 16 An electron-volt is the energy gained by an electron accelerating through a potential difference of one volt. © 2010 Pearson Education, Inc.