before the plates were pulled apart.

Slides:



Advertisements
Similar presentations
Chapter 24 Capacitance, Dielectrics, Electric Energy Storage
Advertisements

Chapter 23: Electrostatic Energy and Capacitance
©1997 by Eric Mazur Published by Pearson Prentice Hall Upper Saddle River, NJ ISBN No portion of the file may be distributed, transmitted.
Ch 26.4 – Energy Stored in a Capacitor – charging a capacitor
Unit 2 Day 3: Electric Energy Storage Electric potential energy stored between capacitor plates Work done to add charge to the capacitor plates Energy.
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
1 W05D2 Dielectrics and Conductors as Shields Today’s Reading Assignment: Course Notes Sections 5.4, 5.6,
PHY 184 Spring 2007 Lecture 14 1/31/ Lecture 14.
Chapter 24 Capacitance, dielectrics and electric energy storage
Chapter 25 Capacitance Key contents Capacitors Calculating capacitance
Fall 2008Physics 231Lecture 4-1 Capacitance and Dielectrics.
Dielectric Materials.
Chapter 17 Electric Potential.
Chapter 23 Capacitance.
Chapter 25 Capacitance.
Capacitance 電容 (Ch. 25) A capacitor 電容器 is a device in which electrical energy is stored. e.g. the batteries in a camera store energy in the photoflash.
Capacitance and Dielectrics
Application – Xerographic Copiers
Capacitance Energy & Dielectrics
I Chapter 25 Electric Currents and Resistance HW7: Due Monday, March 30; Chap.24: Pb.32,Pb.35,Pb.59 Chap.25: Pb.19,Pb.25,Pb.31.
Chapter 26:Capacitance and Dielectrics. Capacitors A capacitor is made up of 2 conductors carrying charges of equal magnitude and opposite sign. The Capacitance.
Tuesday, Oct. 4, 2011PHYS , Fall 2011 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #11 Tuesday, Oct. 4, 2011 Dr. Jaehoon Yu Capacitors in Series.
Bright Storm on Capacitors (Start to minute 7:10).
1 Capacitance and Dielectrics Chapter 27 Physics chapter 27.
Physics for Scientists and Engineers II, Summer Semester Lecture 7: June 3 rd 2009 Physics for Scientists and Engineers II.
When a potential difference of 150 V is applied to the plates of a parallel-plate capacitor, the plates carry a surface charge density of 30.0 nC/cm2.
Copyright © 2009 Pearson Education, Inc. Lecture 5 - Capacitance Capacitors & Dielectrics.
Capacitors as Circuit Elements The most common use of capacitors is in electric circuits. They are used primarily as a means of storing charge, which can.
Capacitance & Dielectrics
Copyright © 2009 Pearson Education, Inc. May Term in Guatemala GDS 3559/STS 3500: Engineering Public Health: An Interdisciplinary Exploration of Community.
Capacitance�and�Dielectrics
Capacitance and Dielectrics
Dielectric Materials. What is a dielectric material? E Dielectric materials consist of polar molecules which are normally randomly oriented in the solid.
Electrical Energy and Capacitance
Electric Potential. Electrostatic Potential Energy and Potential Difference The electrostatic force is conservative – potential energy can be defined.
P WARNING: Exam 1 Week from Thursday. P Class 09: Outline Hour 1: Conductors & Insulators Expt. 4: Electrostatic Force Hour 2: Capacitors.
Wednesday, Feb. 15, 2012 PHYS , Spring 2012 Dr. Jaehoon Yu 1 PHYS 1444 – Section 004 Lecture #9 Wednesday, Feb. 15, 2012 Dr. Jae Yu Capacitors.
Capacitance Chapter 25 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Electric Energy and Capacitance
Capacitors Q D A capacitor is a device that is capable of storing electric charges and thus electric potential energy. => charging Its purpose is to release.
Capacitanc e and Dielectrics AP Physics C Montwood High School R. Casao.
GENERAL PHYSICS LECTURE Chapter 26 CAPACITANCE AND DIELECTRICS Nguyễn Thị Ngọc Nữ PhD: Nguyễn Thị Ngọc Nữ.
Physics 202, Lecture 7 Today’s Topics Capacitance (Ch. 24-II) Review Energy storage in capacitors Dielectric materials, electric dipoles Dielectrics and.
111/16/2015 ELECTRICITY AND MAGNETISM Phy 220 Chapter 4: Capacitors.
Electrical Capacitance:
Copyright © 2009 Pearson Education, Inc. Molecular Description of Dielectrics.
Chapter 16 Electrical Energy AndCapacitance. General Physics Review - Electric Potential for a system of point charges.
Monday Feb. 3, 2014PHYS , Dr. Andrew Brandt 1 PHYS 1442 – Section 004 Lecture #6 Monday February 3, 2014 Dr. Andrew Brandt CH 17 Capacitance Dielectrics.
Capacitance Physics Montwood High School R. Casao.
Chapter 25 Lecture 20: Capacitor and Capacitance.
Capacitance Chapter 25 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Capacitor Engr. Faheemullah Shaikh Lecturer, Department of Electrical Engineering.
Electrical Energy and Capacitance Capacitance. Capacitors and Charge Storage Capacitor – acts as a storehouse of charge and energy –Typically consists.
Capacitance Chapter 25. Capacitance A capacitor consists of two isolated conductors (the plates) with charges +q and -q. Its capacitance C is defined.
Electric Energy and Capacitance
Molecular Description of Dielectrics
-Atomic View of Dielectrics -Electric Dipole in an Electric Field -Partially Filled Capacitors AP Physics C Mrs. Coyle.
Chapter 24 Capacitance Capacitor is a device that stores electrostatic potential energy. A capacitor consists of 2 spatially separated conductors which.
Capacitors Calculating capacitance Energy stored in a capacitor
Chapter 25 Capacitance.
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
11/7/2018.
Introduction to Capacitance
Chapter 25 Capacitance.
General Physics (PHY 2140) Lecture 6 Electrostatics
Capacitance and Dielectrics
Chapter 25 Capacitance Key contents Capacitors Calculating capacitance
Capacitance and Dielectrics Test: Wednesday 2/27
Presentation transcript:

before the plates were pulled apart. Consider a simple parallel-plate capacitor whose plates are given equal and opposite charges and are separated by a distance d. Suppose the plates are pulled apart until they are separated by a distance D > d. The electrostatic energy stored in the capacitor is 1. greater than 2. the same as 3. smaller than before the plates were pulled apart. Q is constant and C decreases with increased separation distance Answer: 1. Since the oppositely charged plates are attracted to each other, work must be done to increase the separation between them. Thus, the electrostatic energy stored in the capacitor increases when the plates are separated. Work must be done on the plates to separate them since the plates are attracted to each other. If you do work on the system you are increasing the potential energy.

Dielectrics and Dipoles When constructing a capacitor we want to have two plates that are separated by a specific distance. If we just fill the capacitor with air it will work, but it may not stand up to physical abuse. What can we do to solve this problem? We can introduce a different material between the plates to add stability, but we also have to be concerned with how this material will affect the capacitance. What type of material would be appropriate? We know it cannot be a conductor, because we would no longer have a capacitor. This means it should be some sort of insulating material. We call these materials Dielectrics. Dielectrics – Materials that are poor conductors of electricity, but support electric fields. Most materials are dielectrics (wood, glass, ceramic, rubber, plastics, wax, dry air, vacuum, etc.). Dielectrics placed in a capacitor are subjected to an electric field. The electric field causes some amount of polarization by either separation of charges or aligning the dipole molecules contained within the material. Dipole – A single molecule that has an excess positive charge on one side and an excess negative charge on the other. In chemistry they call these polar molecules (water, carbon dioxide, hydrogen chloride, etc.).

We can describe a dipole using a dipole moment, which contains information about the magnitude of the charge, the size of the dipole (separation distance between charges) and the orientation of the dipole. The direction of the dipole vector is from negative to positive, to show how an electric field would affect the molecule. The dipole moment is a vector quantity since it contains information on magnitude and direction. +q P – dipole moment 2a If we place a dipole molecule in an electric field, what will happen? p The dipole will align itself with the external electric field. -q The equal magnitude, but oppositely directed forces will cause the dipole to rotate about a point halfway between the two charges. This means that the dipole experiences a torque. E F a F a a F a O Work is done by the electric field on the dipole to rotate it causing a decrease in the stored potential energy. F

If the dielectric we use to fill the capacitor contains dipole (polar) molecules, let us examine how this will affect the capacitance. Non-polar material The polarized materials can be modeled as if there is a charged plate on either side of the dielectric. The induced surface charge density (sind) is less than the surface charge density (s) of the original plates. Hence, the induced electric field (Eind) is less than the initial electric field (E0). The total electric field (E) between the plates of a capacitor containing a dielectric would then be given by: The magnitude of Eind depends on how much polarization can occur in the dielectric. Polar material – made up of dipoles This means that the strength of the electric field for the capacitor with a dielectric must be some fraction of the strength of the electric field without the dielectric. We introduce a new quantity called the Dielectric Constant to represent this ratio of electric field strengths.

Magnitude of Electric field without dielectric k – dielectric constant The dielectric constant is not really a constant! Magnitude of Electric field with dielectric If we want to relate this to a capacitor it is usually more convenient to discuss the potential difference between the plates than the electric field. The dielectric constant can also be written as the ratio of the potential differences. We can now relate the capacitances with and without the dielectric. We can then rewrite the capacitance for a parallel plate capacitor with a dielectric as: The capacitance with the dielectric is larger since k>1.

Maximum voltage rating Above is a selection of common capacitors used in electric circuits. Each of these capacitors use some type of dielectric. When the dielectric is subjected to an electric field we get polarization, but if the electric field is too strong the dielectric can “breakdown” and the capacitor will no longer function as expected. The potential difference across the plates of the capacitor determines the strength of the electric field. Therefore all capacitors have a maximum voltage rating. When exceeded this may ruin the capacitor and even cause it to explode. The maximum electric field that a dielectric can support without breaking down is called the Dielectric Strength. When you exceed the dielectric strength of a material it begins to conduct. Rubber can conduct if you exceed the dielectric strength. Air conducts when you exceed the dielectric strength. (e.g. Lightning)

it would have been if the dielectric were left in place. A dielectric is inserted between the plates of a capacitor. The system is then charged and the dielectric is removed. The electrostatic energy stored in the capacitor is 1. greater than 2. the same as 3. smaller than it would have been if the dielectric were left in place. Cwithout < Cwith, so Uwithout > Uwith and DU increases Work must be done to remove the dielectric since it has become polarized. The now polarized dielectric is attracted to the plate of opposite sign and requires a force to remove it. If you do work on the system you are increasing the potential energy. Answer: 1. The dielectric is polarized when it is between the charged plates. The positively charged dielectric surface is attracted to the negatively charged plate, and the negatively charged dielectric surface is attracted to the positively charged plate. Thus, you must do work to remove the dielectric. As a result, the electrostatic energy stored in the capacitor increases when the dielectric is removed.

A parallel-plate capacitor is attached to a battery that maintains a constant potential difference V between the plates. While the battery is still connected, a glass slab is inserted so as to just fill the space between the plates. The stored energy 1. increases. 2. decreases. 3. remains the same. Cwithout < Cwith, so Uwithout < Uwith and DU increases Work is done by the battery to add more charges to the plates and therefore the potential energy increases. The battery does work on the system. Answer: 1.When the glass slab is between the plates, it becomes polarized, thereby decreasing the magnitude of the electric field. In order for the battery to maintain a constant potential difference across the plates, it must do work to deposit more charge on the plates. Thus, work is done on the system and the stored energy increases.