Physics for Scientists and Engineers, 6e Chapter 25 – Electric Potential.

Slides:



Advertisements
Similar presentations
Chapter 25 Electric Potential.
Advertisements

Electric Potential Energy and the Electric Potential
Which is the correct expression for work
When we have two charged particles interacting, there is a difference between potential energy and electric potential. A.True B.False.
Electric Potential and Field
EE3321 ELECTROMAGENTIC FIELD THEORY
Chapter Fourteen The Electric Field and the Electric Potential
© 2012 Pearson Education, Inc. A beam of electrons (which have negative charge q) is coming straight toward you. You put the north pole of a magnet directly.
Q23.1 When a positive charge moves in the direction of the electric field, Motion +q A. the field does positive work on it and the potential energy increases.
4.1 Exam Date – Wed 2/9 Topics Covered Listed on Class Website Sample Exam from a few years back is also on the web. Today Start Unit 5: Electric Potential.
Chapter 23 Gauss’ Law.
February 16, 2010 Potential Difference and Electric Potential.
Chapter 22 Electric Potential.
Physics 121: Electricity & Magnetism – Lecture 5 Electric Potential Dale E. Gary Wenda Cao NJIT Physics Department.
A Charged, Thin Sheet of Insulating Material
Chapter 25 Electric Potential
Electric Potential Energy PH 203 Professor Lee Carkner Lecture 6.
Topic 9.3 Electric Field, Potential, and Energy
General Physics 2, Lec 6, By/ T.A. Eleyan
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Ch 25 – Electric Potential
Q23.1 When a positive charge moves in the direction of the electric field, 1. the field does positive work on it and the potential energy increases 2.
Lecture 3 Electrical Energy Chapter 16.1  16.5 Outline Potential Difference Electric Potential Equipotential Surface.
Electric Energy and Capacitance
Chapter 16 Electric Energy and Capacitance. Question I Three equal positive charges are placed on the x-axis, one at the origin, one at x = 2 m, and the.
AP Physics C Montwood High School R. Casao
Chapter 24. Electric Potential
Gioko, A. (2007). Eds AHL Topic 9.3 Electric Field, potential and Energy.
Chapter 25 Electric Potential Electrical Potential and Potential Difference When a test charge is placed in an electric field, it experiences a.
Electrostatics: Coulomb’s Law & Electric Fields. Electric Charges  There are two kinds of charges: positive (+) and negative (-), with the following.
Chapter 22 Gauss’s Law Chapter 22 opener. Gauss’s law is an elegant relation between electric charge and electric field. It is more general than Coulomb’s.
President UniversityErwin SitompulEEM 6/1 Dr.-Ing. Erwin Sitompul President University Lecture 6 Engineering Electromagnetics
Wednesday, Jan. 31, PHYS , Spring 2007 Dr. Andrew Brandt PHYS 1444 – Section 004 Lecture #4 Gauss’ Law Gauss’ Law with many charges What.
Tuesday, Sept. 13, 2011PHYS , Fall 2011 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #7 Tuesday, Sept. 13, 2011 Dr. Jaehoon Yu Chapter 22.
Chapter 24 Review on Chapter 23 From Coulomb's Law to Gauss’s Law
CHAPTER OUTLINE 30.1 The Biot–Savart Law 30.2 The Magnetic Force Between Two Parallel Conductors 30.3 Ampère’s Law 30.4 The Magnetic Field of a Solenoid.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Electric potential energy Electric potential Conservation of energy Chapter.
AP Physics C Montwood High School R. Casao
CHAPTER 25 : ELECTRIC POTENTIAL
Chapter 25 Capacitance.
Electrical Energy And Capacitance
Ch – 30 Potential and Field. Learning Objectives – Ch 30 To establish the relationship between and V. To learn more about the properties of a conductor.
Lecture 5: Potential Energy and Electric Potential (Ch. 19)
Thin sheet of any charge distribution
Electric Potential Potential Difference and Electric Potential Potential Differences in a Uniform Electric Field Electric Potential and Potential Energy.
د/ بديع عبدالحليم د/ بديع عبدالحليم
Electrostatics #3 The Electric Field HW #2, last page of handout.
Lecture 5 Dr. Lobna Mohamed Abou El-Magd The Electric Potential.
President UniversityErwin SitompulEEM 6/1 Lecture 6 Engineering Electromagnetics Dr.-Ing. Erwin Sitompul President University
Chapter 21 Electric Potential.
Electric Field.
Lecture 19 Electric Potential
Electric Potential.
Tuesday, Sept. 20, 2011PHYS , Fall 2011 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #9 Tuesday, Sept. 20, 2011 Dr. Jaehoon Yu Chapter 23 Electric.
Electromagnetism Topic 11.1 Electrostatic Potential.
Chapter 25 Electric Potential. Electrical Potential Energy The electrostatic force is a conservative force, thus It is possible to define an electrical.
Wednesday, Feb. 8, 2012PHYS , Spring 2012 Dr. Jaehoon Yu 1 PHYS 1444 – Section 004 Lecture #7 Wednesday, Feb. 8, 2012 Dr. Alden Stradeling Chapter.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Conservation of energy Work and Delta PE Electric potential energy Electric.
1 Electric Potential Reading: Chapter 29 Chapter 29.
Chapter 25 Electric Potential. Like gravity, the electric force is conservative: it has a Potential Energy. A charge in an electric field has electric.
Thursday, Sept. 8, 2011PHYS , Fall 2011 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #6 Thursday, Sept. 8, 2011 Dr. Jaehoon Yu Chapter 21 –Electric.
3/21/20161 ELECTRICITY AND MAGNETISM Phy 220 Chapter2: Gauss’s Law.
Capacitance Chapter 25. Capacitance A capacitor consists of two isolated conductors (the plates) with charges +q and -q. Its capacitance C is defined.
AP Physics ST Induced emf and Electric Fields
Chapter 25 Electric Potential 25.1 Potential Difference and Electric Potential 25.2 Potential Differences in a Uniform Electric Field 25.3 Electric Potential.
QUICK QUIZ 15.1 If a suspended object A is attracted to object B, which is charged, we can conclude that (a) object A is uncharged, (b) object A is charged,
Chapter 25 Electric Potential.
Property of space around a charged object that causes forces on other charged objects Electric Field.
Topic 9.3 Electric Field, Potential, and Energy
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Presentation transcript:

Physics for Scientists and Engineers, 6e Chapter 25 – Electric Potential

In the figure below, two points A and B are located within a region in which there is an electric field. The potential difference ΔV = V B – V A is positive 2.negative 3.zero

When moving straight from A to B, E and ds in Equation 25.3 both point toward the right. Thus, the dot product E · ds is positive and ΔV is negative.

In this figure, a negative charge is placed at A and then moved to B. The change in potential energy of the charge–field system for this process is positive 2.negative 3.zero

From Equation 25.3, ΔU = q 0 ΔV, so if a negative test charge is moved through a negative potential difference, the potential energy is positive. Work must be done to move the charge in the direction opposite to the electric force on it.

The labeled points of the figure below are on a series of equipotential surfaces associated with an electric field. Rank (from greatest to least) the work done by the electric field on a positively charged particle that moves along the following transitions A -> B, B -> C, C -> D, D -> E 2. A -> B, D -> E, B -> C, C -> D 3. B -> C, C -> D, A -> B, D -> E 4. D -> E, C -> D, B -> C, A -> B

Moving from B to C decreases the electric potential by 2 V, so the electric field performs 2 J of work on each coulomb of positive charge that moves. Moving from C to D decreases the electric potential by 1 V, so 1 J of work is done by the field. It takes no work to move the charge from A to B because the electric potential does not change. Moving from D to E increases the electric potential by 1 V, and thus the field does –1 J of work per unit of positive charge that moves.

For the equipotential surfaces in this figure, what is the approximate direction of the electric field? Out of the page 2.Into the page 3.Toward the right edge of the page 4.Toward the left edge of the page 5.Toward the top of the page 6.Toward the bottom of the page

The electric field points in the direction of decreasing electric potential.

A spherical balloon contains a positively charged object at its center. As the balloon is inflated to a greater volume while the charged object remains at the center, the electric potential at the surface of the balloon will increase 2.decrease 3.remain the same.

The electric potential is inversely proportional to the radius (see Eq ).

Recall that the spherical balloon from the last question contains a positively charged object at its center. As the balloon is inflated to a greater volume while the charged object remains at the center, the electric flux through the surface of the balloon will increase 2.decrease 3.remain the same.

Because the same number of field lines passes through a closed surface of any shape or size, the electric flux through the surface remains constant.

In Figure 25.10a, take q 1 to be a negative source charge and q 2 to be the test charge. If q 2 is initially positive and is changed to a charge of the same magnitude but negative, the potential at the position of q 2 due to q increases 2.decreases 3.remains the same

The potential is established only by the source charge and is independent of the test charge.

Consider the situation from the last question again. When q 2 is changed from positive to negative, the potential energy of the two-charge system increases 2.decreases 3.remains the same

The potential energy of the two-charge system is initially negative, due to the products of charges of opposite sign in Equation When the sign of q 2 is changed, both charges are negative, and the potential energy of the system is positive.

In a certain region of space, the electric potential is zero everywhere along the x axis. From this we can conclude that the x component of the electric field in this region is zero 2.in the x direction 3.in the – x direction.

If the potential is constant (zero in this case), its derivative along this direction is zero.

In a certain region of space, the electric field is zero. From this we can conclude that the electric potential in this region is zero 2.constant 3.positive 4.negative

If the electric field is zero, there is no change in the electric potential and it must be constant. This constant value could be zero but does not have to be zero.