Physics Lecture 14: MON 29 SEP

Similar documents
Last Time emphasis on E-field. Potential of spherical conductor. Quick quiz. Connected spheres. Varying E-fields on conductor.

Physics 1402: Lecture 7 Today s Agenda

Reading from Young & Freedman: For this topic, read the introduction to chapter 24 and sections 24.1 to 24.5.

CAPACITORS AND DIELECTRICS

Homework Assignment 5 Solution Set

Phys 201 Midterm 1 S. Nergiz, E.Oğuz, C. Saçlıoğlu T. Turgut Fall '01 No :. Name :. Total Grade :. Grade :. y=a. x=-a +q. x=a -q +q. +Q r.

Physics 1B schedule Winter Instructor: D.N. Basov Ch18: 1,3,5,7,13,17,21,26,31,33,35,

Problems for HW X. C. Gwinn. November 30, 2009

ELETROSTATICS Part II: BASICS

A, Electromagnetic Fields Final Exam December 14, 2001 Solution

PH 102 Exam I Solutions

Phys102 General Physics II

Physics 2135 Exam 1 September 23, 2014

Physics 3323, Fall 2016 Problem Set 7 due Oct 14, 2016

CLASS XII PHYSICS. (a) 30 cm, 60 cm (b) 20 cm, 30 cm (c) 15 cm, 20 cm (d) 12 cm, 15 cm. where

Capacitance and Dielectrics

Lecture 10: PN Junction & MOS Capacitors

Lecture 5 Capacitance Ch. 25

Exam 1 Solutions (1) C, D, A, B (2) C, A, D, B (3) C, B, D, A (4) A, C, D, B (5) D, C, A, B

Physics 2135 Exam 1 February 14, 2017

Exam 1 September 21, 2012 Instructor: Timothy Martin

Lecture 1: Electrostatic Fields

TIME VARYING MAGNETIC FIELDS AND MAXWELL S EQUATIONS

Sample Exam 5 - Skip Problems 1-3

Jackson 2.26 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Physics 24 Exam 1 February 18, 2014

PHYS102 - Electric Energy - Capacitors

Today in Physics 122: work, energy and potential in electrostatics

Lecture 13 - Linking E, ϕ, and ρ

Homework Assignment 3 Solution Set

Reference. Vector Analysis Chapter 2

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory 2. Diffusion-Controlled Reaction

Physics 202, Lecture 14

Electric Potential. Electric Potential Video: Section 1 4. Electric Fields and WORK 9/3/2014. IB Physics SL (Year Two) Wednesday, September 3, 2014

Summary of equations chapters 7. To make current flow you have to push on the charges. For most materials:

Physics 202, Lecture 10. Basic Circuit Components

200 points 5 Problems on 4 Pages and 20 Multiple Choice/Short Answer Questions on 5 pages 1 hour, 48 minutes

Designing Information Devices and Systems I Discussion 8B

ECE 307: Electricity and Magnetism Spring 2010

Chapter 6 Electrostatic Boundary Value Problems. Dr. Talal Skaik

Homework Assignment 9 Solution Set

I1 = I2 I1 = I2 + I3 I1 + I2 = I3 + I4 I 3

Section 20.1 Electric Charge and Static Electricity (pages )

Review of Gaussian Quadrature method

Summary: Method of Separation of Variables

Conservation Law. Chapter Goal. 6.2 Theory

If we have a function f(x) which is well-defined for some a x b, its integral over those two values is defined as

Physics Jonathan Dowling. Lecture 9 FIRST MIDTERM REVIEW

dy ky, dt where proportionality constant k may be positive or negative

Mathematics Number: Logarithms

Resistors. Consider a uniform cylinder of material with mediocre to poor to pathetic conductivity ( )

Ch 26 - Capacitance! What s Next! Review! Lab this week!

DIRECT CURRENT CIRCUITS

Chapter 4 Contravariance, Covariance, and Spacetime Diagrams

Chapter E - Problems

Lecture 3. In this lecture, we will discuss algorithms for solving systems of linear equations.

EMF Notes 9; Electromagnetic Induction ELECTROMAGNETIC INDUCTION

Math 211A Homework. Edward Burkard. = tan (2x + z)

ragsdale (zdr82) HW2 ditmire (58335) 1

Instructor(s): Acosta/Woodard PHYSICS DEPARTMENT PHY 2049, Fall 2015 Midterm 1 September 29, 2015

- 5 - TEST 2. This test is on the final sections of this session's syllabus and. should be attempted by all students.

13: Diffusion in 2 Energy Groups

The graphs of Rational Functions

Phys 4321 Final Exam December 14, 2009

When you set an old-fashioned spring mousetrap or pull back the string

Measuring Electron Work Function in Metal

1B40 Practical Skills

1 Online Learning and Regret Minimization

Designing Information Devices and Systems I Spring 2018 Homework 8

Lecture 2: January 27

Name Solutions to Test 3 November 8, 2017

10/25/2005 Section 5_2 Conductors empty.doc 1/ Conductors. We have been studying the electrostatics of freespace (i.e., a vacuum).

(1) It increases the break down potential of the surrounding medium so that more potential can be applied and hence more charge can be stored.

Density of Energy Stored in the Electric Field

Improper Integrals. Type I Improper Integrals How do we evaluate an integral such as

Magnetic forces on a moving charge. EE Lecture 26. Lorentz Force Law and forces on currents. Laws of magnetostatics

Prof. Anchordoqui. Problems set # 4 Physics 169 March 3, 2015

HW3, Math 307. CSUF. Spring 2007.

p(t) dt + i 1 re it ireit dt =

Name Class Date. Match each phrase with the correct term or terms. Terms may be used more than once.

UNIT 4:Capacitors and Dielectric

20 MATHEMATICS POLYNOMIALS

Chapter 0. What is the Lebesgue integral about?

Heavy tail and stable distributions

Version 001 Exam 1 shih (57480) 1

ADVANCEMENT OF THE CLOSELY COUPLED PROBES POTENTIAL DROP TECHNIQUE FOR NDE OF SURFACE CRACKS

University of Alabama Department of Physics and Astronomy. PH126: Exam 1

The Velocity Factor of an Insulated Two-Wire Transmission Line

How do we solve these things, especially when they get complicated? How do we know when a system has a solution, and when is it unique?

Interpreting Integrals and the Fundamental Theorem

7.2 The Definite Integral

This final is a three hour open book, open notes exam. Do all four problems.

Farey Fractions. Rickard Fernström. U.U.D.M. Project Report 2017:24. Department of Mathematics Uppsala University

CHAPTER 20: Second Law of Thermodynamics

Lecture 7 notes Nodal Analysis

Consider a potential problem in the half-space dened by z 0, with Dirichlet boundary conditions on the plane z = 0 (and at innity).

Intro to Nuclear and Particle Physics (5110)

Math 8 Winter 2015 Applications of Integration

State space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies

4 7x =250; 5 3x =500; Read section 3.3, 3.4 Announcements: Bell Ringer: Use your calculator to solve

Transcription:

Physics 2113 Physics 2113 Lecture 14: MON 29 SEP CH25: Cpcitnce

Von Kleist ws le to store electricity in the jr. Unknowingly, he h ctully invente novel evice to store potentil ifference. The wter in the jr forme the inner coting n his hns forme the outer coting of this evice, with glss s the meium isolting two conuctors (his oy n wter). Von Kleist switche on his genertor, chrge flowe to the glss jr, n he ecie to remove the glss jr from the mchine. Surprisingly, he receive n electric shock! Why?

Potentil irectly les to work. If evice cn store the potentil ifference, we cn use it to o necessry work. Cpcitors (or conensers s Volt clle them) re exmples of such evices. Potentil ifference generte t isolte chrge surfces, les to genertion of sttic electric fiel etween the surfces, which stores the energy. A ttery is evice tht mintins constnt potentil ifference cross its ens (through chemicl mens). A circuit is pth long which chrge flows. A switch is evice which if open oes not llow flow of chrge. Then the circuit is si to e open. If switch is close, circuit is close. +

When the switch is open, the circuit is incomplete n there is no flow of chrge. When the switch is close, the circuit is complete n electrons from plte h re ttrcte to the positive terminl of ttery, mking plte h positively chrge. Similrly, plte l ecomes negtively chrge. After some time, when the pltes re fully chrge, the potentil ifference etween the pltes is sme s V. There is no more flow of chrge.

+ If the prllel pltes were unchrge n lter the ttery ws connecte to them, it will tke electrons from the + plte towrs the - plte. The prllel pltes re the simplest exmple of cpcitor. They pck n electric fiel mong them. Appropritely constructe, the fiel cn e very intense. The chrge on ech plte is proportionl to the potentil mong the pltes: q CV Whenever these quntities re proportionl, the constnt C is efine s the cpcitnce of the evice in question. This unit is typiclly too lrge. Most common re: Units: Coulom [ C] Volt Fr MicroFr µ F 1 PicoFr pf 1-12 -6 F F (MicroMicroF) NnoFr nf 1-9 F

The cpcitnce of evice is completely etermine y the chrcteristics of the evice (geometry, mterils). It oes not epen on pplie potentils, chrges or fiels. Computing cpcitnce: Strtegy: compute V s function of q, re off the proportionlity fctor! Prllel pltes: + + + + + + + E - - - - - - - If the seprtion is smll compre to the size of the pltes we cn pproximte the fiel for tht of infinite plnes: V σ A E!! E s A E A Are of pltes. A V C C

Motheror of Iphone S

Interior of 1989 Snyo Wlkmn Vrile cpcitor (tuner) Cermic cpcitors Tntlum Cpcitor Electrolytic cpcitors

Electrolytic (194-7) Electrolytic (new) Pper (194-7) Tigers Vrile ir, mic Tntlum (198 on) Cermic (193 on) Mic (193-5

Cylinricl pltes: -q +q r Agin, we pproximte the fiel for tht of n infinite cyliner. To compute this, we surroun the interior cyliner with cylinricl Gussin surfce. V!! E A V L 2π rl E!! E l Er E 2π L 2π rl r r 2π L 2π L [ ln( ) ln( ) ] ln

L ln 2 V π so L C ln 2 π Cylinricl cpcitor n rius lrge, seprtion is smll, If for lrge. 1 ln ln ln ln + + + like plne cpcitor. 2 A L C π

Sphericl cpcitor: V Similr to cyliner,!! E A E V 2 4π r!! E l 4π 2 r E Er -q +q r r 1 1 1 2 4π r 4π r 4π π 4 Now V V V, therefore C 4π Limit cses: If R, noting tht we hve, C 2 4π R A 4π R 2, A Plnr If, C 4π Cpcity of conucting sphere

Dielectrics: We know tht in insultors, electrons cnnot move freely s in conuctors. However, they o exhiit limite rnge of motion. Molecules re not sphericlly symmetric n they tilt in response to n pplie electric fiel. As ll polriztion effects, it hs the consequence of iminishing the fiel insie the insultor (extreme cse: conuctor, no fiel). Tht is, if one inserts n insultor etween the pltes of cpcitor, ue to polriztion effects the fiel (n the potentil) will e smller for given chrge, thn if one h vcuum mong the pltes. q CV Implies tht q is fixe, V is smller, therefore C is igger! Inserting ielectric is prcticl wy of incresing the cpcitnce of cpcitor. It lso llows to tolerte higher V mong pltes without sprks flying etween them (some ielectrics rek own less thn ir).

Different types of Dielectrics: Polr ielectrics: The molecules of these mterils hve permnent electric ipole moment. These electric ipoles lign long the electric fiel when it is externlly pplie on the mteril. Non-Polr ielectrics: Molecules cquire ipole moment when plces in the electric fiel. It is cuse ecuse of stretching of the molecules.

Given two ienticl cpcitors, one with ielectric n the other in vcuum, we write, κ Ciel κ C vcuum for prllel plte cpcitor : C A iel So we cn sor the constnt κ in the efinition of κ All equtions we erive up to now re correct in the presence of ielectrics if one replces in plce of! Some vlues: κ κ vcuum ir 1 1.54 κ κ pper wter 35 8 Electric fiel of point chrge in ielectric E q 4π r 2 Guss lw:!! E s q q q q' If one uses, there is no nee to tke into ccount explicitly inuce chrges.

Summry: We ve seen wht cpcitor is: evice tht pcks electric fiel in confine region. Next clss we will lern wht hppens when you connect more thn one such evice, n how they ctully store energy.