Electric Potential. Electrostatic Potential Energy and Potential Difference The electrostatic force is conservative – potential energy can be defined.

Slides:



Advertisements
Similar presentations
Electric Potential Energy and the Electric Potential
Advertisements

before the plates were pulled apart.
Chapter 24 Capacitance, Dielectrics, Electric Energy Storage
Physics 152 Walker, Chapter 20 Electrostatic Potential Energy Electrostatic Potential.
© 2014 Pearson Education, Inc. This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Copyright © 2009 Pearson Education, Inc. Dielectrics.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Chapter 17 Electric Potential.
Electric Potential Chapter 23 opener. We are used to voltage in our lives—a 12-volt car battery, 110 V or 220 V at home, 1.5 volt flashlight batteries,
Lecture 4 Capacitance and Capacitors Chapter 16.6  Outline Definition of Capacitance Simple Capacitors Combinations of Capacitors Capacitors with.
An equipotential surface is a surface on which the electric potential is the same everywhere. Since the potential at a distance r from an isolated point.
Electric Potential AP Physics: M. Blachly Textbook: 17:1-3.
17-7 Capacitance A device that stores electric charge Two plates that are separated by an insulator Used in electronic circuits Store charge that can later.
February 16, 2010 Potential Difference and Electric Potential.
1 Capacitance and Dielectrics Chapter 27 Physics chapter 27.
Capacitance Physics Department, New York City College of Technology.
Copyright © 2009 Pearson Education, Inc. Lecture 5 - Capacitance Capacitors & Dielectrics.
Copyright © 2009 Pearson Education, Inc. Lecture 4 – Electricity & Magnetism b. Electric Potential.
Chapter 18 – Electric Potential and Capacitance Section 1 Electric Potential Energy.
Capacitance & Dielectrics
FCI1 CHAPTER OUTLINE 1. Definition of Capacitance 2. Calculating Capacitance 3. Combinations of Capacitors 4. Energy Stored in a Charged Capacitor.
Chapter 24 Capacitance, Dielectrics, Electric Energy Storage
Electrical Energy and Capacitance
Electric Potential, Electric Energy and Capacitance
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is.
Electric Potential and Electric Energy Chapter 17.
Chapter 17 Electric Potential. Objectives: The students will be able to: Given the dimensions, distance between the plates, and the dielectric constant.
1 My Chapter 17 Lecture Outline. 2 Chapter 17: Electric Potential Electric Potential Energy Electric Potential How are the E-field and Electric Potential.
Electric Potential AP Physics Chapter 17. Electric Charge and Electric Field 17.1 Electric Potential Energy and Potential Difference.
1 Electric Potential Reading: Chapter 21 Chapter 21.
Chapter 17 Electric Energy and Capacitance. Work and Potential Energy For a uniform field between the two plates As the charge moves from A to B, work.
Chapter 18 Electrical Energy and Capacitance. Chapter 18 Objectives Electrical potential Electric Potential from a Point Charge Capacitance Parallel Plate.
Electrostatics. Electric Charge and Electric Field.
Lecture 5 Potential Difference Capacitance Combinations of Capacitors
Electric Potential and Electric Energy; Capacitance Adapted from Giancoli Physics.
Chapter 17 Electric Potential.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Electric potential energy Electric potential Conservation of energy Capacitors.
Electric Energy and Capacitance
PHYS 1110 Lecture 5 Professor Stephen Thornton September 13, 2012.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Electric potential energy Electric potential Conservation of energy Chapter.
Weds., Jan. 29, 2014PHYS , Dr. Andrew Brandt 1 PHYS 1442 – Section 004 Lecture #5 Wednesday January 29, 2014 Dr. Andrew Brandt CH 17 Electric Potential.
111/16/2015 ELECTRICITY AND MAGNETISM Phy 220 Chapter 4: Capacitors.
Chapter 16 Electrical Energy and Capacitance. Objectives Electrical potential Electric Potential from a Point Charge Electron Volt Capacitance Parallel.
Static Electricity, Electric Forces, Electric Fields, Electric Potential Energy, Electric Potential, Capacitors.
Chapter 16 Electrical Energy and Capacitance Conceptual Quiz Questions.
Capacitance Physics Montwood High School R. Casao.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Electric potential energy Electric potential Conservation of energy Equipotential.
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Capacitor Engr. Faheemullah Shaikh Lecturer, Department of Electrical Engineering.
Static Electricity, Electric Forces, Electric Fields
Chapter 20 Electric Potential and Electric Potential Energy.
Chapter 13 Electric Energy and Capacitance. Electric Potential Energy The electrostatic force is a conservative force It is possible to define an electrical.
Capacitor Device that can store electric charge Two conducting objects are placed near one another but not touching Power source charges up the plates,
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Electric Energy and Capacitance
Capacitance, Polarization and Dielectrics
Chapter 17 Electric Potential
Electric Potential AP Physics Chapter 17.
Electric Potential and Capacitance.
17.1 Electric potential Energy
Physics: Principles with Applications, 6th edition
Phys102 Lecture 7/8 Capacitors
Chapter 17 Electric Potential
An equipotential surface is a surface on which the electric potential is the same everywhere. Since the potential at a distance r from an isolated point.
Chapter 23 Electric Potential.
Chapter 17 Electric Potential.
Capacitor Is a device that stores energy by maintaining a separation between positive and negative charge. Compare stored energy / charge to a bucket.
Presentation transcript:

Electric Potential

Electrostatic Potential Energy and Potential Difference The electrostatic force is conservative – potential energy can be defined Change in electric potential energy is negative of work done by electric force:

Electrostatic Potential Energy and Potential Difference Electric potential is defined as potential energy per unit charge: Unit of electric potential: the volt ( V ). 1 V = I J / C.

Electrostatic Potential Energy and Potential Difference Only changes in potential can be measured, allowing free assignment of V = 0.

Electrostatic Potential Energy and Potential Difference Analogy between gravitational and electrical potential energy:

Equipotential Lines An equipotential is a line or surface over which the potential is constant. Electric field lines are perpendicular to equipotentials. The surface of a conductor is an equipotential.

Equipotential Lines

The Electron Volt, a Unit of Energy One electron volt (eV) is the energy gained by an electron moving through a potential difference of one volt.

Electric Potential Due to Point Charges The electric potential due to a point charge can be derived:

Electric Potential Due to Point Charges These plots show the potential due to (a) positive and (b) negative charge.

Electric Potential Due to Point Charges Using potentials instead of fields can make solving problems much easier – potential is a scalar quantity, whereas the field is a vector.

Capacitance A capacitor consists of two conductors that are close but not touching. A capacitor has the ability to store electric charge.

Capacitance Parallel-plate capacitor connected to battery. (b) is a circuit diagram.

Capacitance When a capacitor is connected to a battery, the charge on its plates is proportional to the voltage: The quantity C is called the capacitance. Unit of capacitance: the farad ( F ) 1 F = 1 C / V

Capacitance The capacitance does not depend on the voltage; it is a function of the geometry and materials of the capacitor. For a parallel-plate capacitor:

A parallel–plate capacitor has a capacitance C o. A second parallel–plate capacitor has plates with twice the area and twice the separation. The capacitance of the second capacitor is most nearly (A) ¼C o (B) ½C o (C) C o (D) 2C o (E) 4C o

A parallel–plate capacitor has a capacitance C o. A second parallel–plate capacitor has plates with twice the area and twice the separation. The capacitance of the second capacitor is most nearly (A) ¼C o (B) ½C o (C) C o (D) 2C o (E) 4C o

Two square parallel–plate capacitors of capacitances C 1 and C 2 have the dimensions shown in the diagrams above. The ratio of C 1 to C 2 is (A) 1 to 4 (B) 1 to 2 (C) 1 to 1 (D) 2 to 1 (E) 4 to 1

Dielectrics A dielectric is an insulator, and is characterized by a dielectric constant K. Capacitance of a parallel-plate capacitor filled with dielectric:

Dielectrics Dielectric strength is the maximum field a dielectric can experience without breaking down.

Dielectrics The molecules in a dielectric tend to become oriented in a way that reduces the external field.

Dielectrics This means that the electric field within the dielectric is less than it would be in air, allowing more charge to be stored for the same potential.

A sheet of mica is inserted between the plates of an isolated charged parallel–plate capacitor. Which of the following statements is true? (A)The capacitance decreases. (B) The potential difference across the capacitor decreases. (C) The energy of the capacitor does not change. (D) The charge on the capacitor plates decreases (E) The electric field between the capacitor plates increases.

A sheet of mica is inserted between the plates of an isolated charged parallel–plate capacitor. Which of the following statements is true? (A)The capacitance decreases. (B) The potential difference across the capacitor decreases. (C) The energy of the capacitor does not change. (D) The charge on the capacitor plates decreases (E) The electric field between the capacitor plates increases. Since the capacitor is isolated, Q remains constant. Filling the place with oil (a dielectric) will increase the capacitance, causing the potential (V = Q/C) to decrease.

Which of the following capacitors, each of which has plates of area A, would store the most charge on the top plate for a given potential difference V?

The capacitor with the largest capacitance will store the most charge. C =  0 A/d where  glass >  air and  vacuum so E

Storage of Electric Energy A charged capacitor stores electric energy; the energy stored is equal to the work done to charge the capacitor.

A 20 μF parallel–plate capacitor is fully charged to 30 V. The energy stored in the capacitor is most nearly (A)9 × 10 3 J (B) 9 × 10 –3 J (C) 6 × 10 –4 J (D) 2 × 10 –4 J (E) 2 × 10 –7 J

A 20 μF parallel–plate capacitor is fully charged to 30 V. The energy stored in the capacitor is most nearly (A)9 × 10 3 J (B) 9 × 10 –3 J (C) 6 × 10 –4 J (D) 2 × 10 –4 J (E) 2 × 10 –7 J U C = ½ CV 2

A potential difference V is maintained between two large, parallel conducting plates. An electron starts from rest on the surface of one plate and accelerates toward the other. Its speed as it reaches the second plate is proportional to (A) 1/V (B) (C) √V (D) V (E) V 2

A potential difference V is maintained between two large, parallel conducting plates. An electron starts from rest on the surface of one plate and accelerates toward the other. Its speed as it reaches the second plate is proportional to (A) 1/V (B) (C) √V (D) V (E) V 2 W = K = q  V and K = ½ mv 2