Outline. Show that the electric field strength can be calculated from the pd.

Slides:



Advertisements
Similar presentations
Capacitance and Dielectrics In mechanics we are used to devices which store potential energy Is there a way to store electric potential energy Capacitors.
Advertisements

1/29/07184 Lecture 121 PHY 184 Spring 2007 Lecture 12 Title: Capacitor calculations.
Chapter 25. Capacitance What is Physics? Capacitance
EE3321 ELECTROMAGENTIC FIELD THEORY
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Chapter 25 Capacitance Key contents Capacitors Calculating capacitance
Physics 121: Electricity & Magnetism – Lecture 6 Capacitance
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Chapter 25 Capacitance.
Capacitance Energy & Dielectrics
February 16, 2010 Potential Difference and Electric Potential.
Capacitance and Dielectrics AP Physics C. Commercial Capacitor Designs Section
Capacitance Definition Parallel Plate Capacitors Cylindrical Capacitor
Physics 1402: Lecture 7 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
1 Fall 2004 Physics 3 Tu-Th Section Claudio Campagnari Lecture 12: 4 Nov Web page:
Chapter 26 Capacitance and Dielectrics. Concept Question 1.
1 TOPIC 5 Capacitors and Dielectrics. 2 Capacitors are a means of storing electric charge (and electric energy) It takes energy to bring charge together.
Today’s agenda: Capacitance. You must be able to apply the equation C=Q/V. Capacitors: parallel plate, cylindrical, spherical. You must be able to calculate.
Gauss’ Law. Class Objectives Introduce the idea of the Gauss’ law as another method to calculate the electric field. Understand that the previous method.
EXERCISES Try roughly plotting the potential along the axis for some of the pairs Exercises on sheet similar to this.
Copyright © 2009 Pearson Education, Inc. Various Capacitors Chapter 24 : Capacitance & Dielectrics. (in the book by Giancoli). Chapter 26 in our book.
Physics.
Capacitance and Geometry
III.A 3, Gauss’ Law.
Definitions & Examples d A a b L C 1 C 2 a b C 3 C ab 
Capacitance and Dielectrics áCapacitance áCapacitors in combination #Series #Parallel áEnergy stored in the electric field of capacitors and energy density.
1 Electric Potential Reading: Chapter 21 Chapter 21.
Capacitance Chapter 25 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
CHAPTER 26 : CAPACITANCE AND DIELECTRICS
-Capacitors and Capacitance AP Physics C Mrs. Coyle.
Capacitanc e and Dielectrics AP Physics C Montwood High School R. Casao.
Capacitance PHY 2049 Chapter 25 Chapter 25 Capacitance In this chapter we will cover the following topics: -Capacitance C of a system of two isolated.
Obtaining Electric Field from Electric Potential Assume, to start, that E has only an x component Similar statements would apply to the y and z.
Chapter 25 Capacitance.
Chapter 23 Electric Potential. Basics The potential due to an electric dipole is just the sum of the potentials due to each charge, and can be calculated.
Electric field, Electric Potential Difference and Capacitance.
CHAPTER 26 : CAPACITANCE AND DIELECTRICS
1 Capacitance and Capacitors Capacitance:  Any volume (material) that has net charge in it produces electric potential around it (Gauss’ Law).  The ratio.
Capacitance Chapter 25 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Electric Potential: Charged Conductor
President UniversityErwin SitompulEEM 9/1 Lecture 9 Engineering Electromagnetics Dr.-Ing. Erwin Sitompul President University
Capacitance Chapter 25. Capacitance A capacitor consists of two isolated conductors (the plates) with charges +q and -q. Its capacitance C is defined.
Conductors and Dielectrics UNIT II 1B.Hemalath AP-ECE.
Capacitor Two conductors carrying charges of equal magnitude but opposite sign form a capacitor. +Q -Q A parallel plate capacitor is a particularly common.
Physics 212 Lecture 7, Slide 1 Physics 212 Lecture 7 Conductors and Capacitance.
EXAMPLES OF SOLUTION OF LAPLACE’s EQUATION NAME: Akshay kiran E.NO.: SUBJECT: EEM GUIDED BY: PROF. SHAILESH SIR.
Chapter 25 Capacitance In this chapter we will cover the following topics: -Capacitance C of a system of two isolated conductors.
Chapter 25 Capacitance In this chapter we will cover the following topics: -Capacitance C of a system of two isolated conductors.
GOVERNMENT ENGINEERING COLLEGE GODHRA
Capacitance & Dielectrics
Capacitors: parallel plate, cylindrical, spherical.
Electric Potential Energy of a Charge (continued)
Capacitance and Dielectric
Consider two conductors carrying charges of equal magnitude but of opposite sign, Such a combination of two conductors is called a capacitor. The.
Capacitors Calculating capacitance Energy stored in a capacitor
Capacitance (Chapter 26)
Chapter 25 Capacitance.
Lecture 5 : Conductors and Dipoles
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Chapter 25 Capacitance.
Physics 014 Capacitance.
Electric Potential: Charged Conductor
Exercises on sheet similar to this
Chapter 6 Dielectrics and Capacitance Capacitance Now let us consider two conductors embedded in a homogenous dielectric. Conductor M2 carries a total.
Chapter 25 Capacitance Key contents Capacitors Calculating capacitance
Consider two conductors carrying charges of equal magnitude but of opposite sign, Such a combination of two conductors is called a capacitor. The capacitance.
Electrical Energy and Current
Capacitance PHY 2049 Chapter 25.
Capacitance PHY 2049 Chapter 25.
Presentation transcript:

Outline

Show that the electric field strength can be calculated from the pd.

Class Objectives Show and apply an equation for calculating the electric field strength from the pd.

Calculating the field from the Potential Previously we calculated the potential at a point given the electric field along a given path. Now we wish to do the opposite. That is, to find the electric field given the potential.

Calculating the field from the Potential Consider a test charge q 0 that moves through a displacement ds from one equipotential to another. + E ds s

Calculating the field from the Potential It can be shown that,

Calculating the field from the Potential It can be shown that, In general, In the simple case where the electric field is constant,

Example The electric potential at any point from the central axis of a uniformly charged disc is From this equation derive the expression for the electric field at any point from the central axis.

Example

Capacitance

Outline Introduce capacitors as an application where the method of electric field strength being calculated from the pd will be used.

Capacitance A capacitor is a device which stores energy as potential energy in an electric field.

Capacitance A capacitor is a device which stores energy as potential energy in an electric field. They are used in the VCR, TV, radio etc.

Capacitance A basic capacitor consists of two charge conductors of any shape.

Capacitance When charged the conductors have opposite charge +q and –q.

Capacitance When charged the conductors have opposite charge +q and –q. A common arrangement is the parallel plate capacitor.

Capacitance The charge on a plate is given by,

Capacitance The charge on a plate is given by, Clearly, SI unit is the farad. 1 farad = 1 F = 1 coulomb per volt = 1 C/V

Calculating the Capacitance We now look at calculating the capacitance for a given geometry. Assuming a charge q on the plates, we calculate E. And then V. Given q and V we can determine C.

Capacitance Calculating E. To calculate E we use gauss’ law.

Capacitance We draw a Gaussian surface enclosing the charge on the positive plate.

Capacitance Recall gauss’ law,

Capacitance Recall gauss’ law, Where q is the charge enclosed.

Capacitance Recall gauss’ law, Where q is the charge enclosed. Since E is constant and E and dA are parallel:

Capacitance Calculating V. Recall,

Capacitance Calculating V. Recall, The integral is always in the direction of the electric field. Integrating we get,

Capacitance The two equations produced hold for any geometry.

Capacitance The two equations produced hold for any geometry. Let us continue for the case of a parallel plate capacitor.

Capacitance The two equations produced hold for any geometry. Let us continue for the case of a parallel plate capacitor. Recall:

Capacitance The two equations produced hold for any geometry. Let us continue for the case of a parallel plate capacitor. Recall: Integrating the first equation we get,

Capacitance Substituting for q and V we get that,

Cylindrical Capacitor

Capacitance A cross section of the cylindrical capacitor of length L formed by coaxial cylinders of radii a and b is shown below. a b +q -q

Capacitance Assume L >> b so that fringe effects are negligible. Each plate contains charge q.

Capacitance First determine E. To find E we draw a cylindrical Gaussian surface between the two plates. a b +q -q r

Capacitance Using Gauss’ law we get that, Alt

Capacitance Determining V. Again

Capacitance Determining V. Again Substitute for E,

Capacitance Determining V. Again Substitute for E,

Capacitance Therefore,

Spherical Capacitor

Capacitance Now consider the case of a capacitor made up of two concentric spherical shells of radii a and b. a b +q -q

Capacitance In this case to find E we draw a spherical Gaussian surface between the two shells. a b +q -q r

Capacitance Using Gauss’ law we get that, Alt

Capacitance Determining V. After substituting for E we get,

Capacitance Determining V. After substituting for E we get,

Capacitance Determining V. After substituting for E we get, Which we make more tidy to give,

Capacitance Finally using the equation for the capacitance we get,

Exercise Review capacitors in combination.