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

Similar documents
(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.

Chapter 25 Electric Potential

Electric Potential. and Equipotentials

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3

General Physics (PHY 2140)

Lecture 11: Potential Gradient and Capacitor Review:

(A) 6.32 (B) 9.49 (C) (D) (E) 18.97

Physics 604 Problem Set 1 Due Sept 16, 2010

Solutions to Midterm Physics 201

U>, and is negative. Electric Potential Energy

Chapter 25: Current, Resistance and Electromotive Force. Charge carrier motion in a conductor in two parts

Chapter 25: Current, Resistance and Electromotive Force. ~10-4 m/s Typical speeds ~ 10 6 m/s

Physics Lecture 14: MON 29 SEP

Physics 11b Lecture #11

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is:

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

Chapter 21: Electric Charge and Electric Field

Physics 1402: Lecture 7 Today s Agenda

Electricity & Magnetism Lecture 6: Electric Potential

Electric Potential Energy

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface

This immediately suggests an inverse-square law for a "piece" of current along the line.

Chapter 28 Sources of Magnetic Field

ELECTROSTATICS. Syllabus : Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road PE 1

Lecture 4. Electric Potential

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

Algebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016

r = (0.250 m) + (0.250 m) r = m = = ( N m / C )

Answers to test yourself questions

ELECTRO - MAGNETIC INDUCTION

CHAPTER 29 ELECTRIC FIELD AND POTENTIAL EXERCISES

Fluids & Bernoulli s Equation. Group Problems 9

Designing Information Devices and Systems I Discussion 8B

CAPACITORS AND DIELECTRICS

CHAPTER? 29 ELECTRIC FIELD AND POTENTIAL EXERCISES = 2, N = (5.6) 1 = = = = = Newton

Ch.9. Electromagnetic Induction

Prof. Anchordoqui Problems set # 12 Physics 169 May 12, 2015

Important design issues and engineering applications of SDOF system Frequency response Functions

ELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy:

Work, Potential Energy, Conservation of Energy. the electric forces are conservative: ur r

π,π is the angle FROM a! TO b

Chapter 2: Electric Field

PHYS 2421 Fields and Waves

Continuous Charge Distributions

Optimization. x = 22 corresponds to local maximum by second derivative test

This chapter is about energy associated with electrical interactions. Every

Electric Potential. chapter

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD

PX3008 Problem Sheet 1

Physics 2135 Exam 1 February 14, 2017

SPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018.

PH 102 Exam I Solutions

Chapter 23 Electrical Potential

6. Gravitation. 6.1 Newton's law of Gravitation

4. Compare the electric force holding the electron in orbit ( r = 0.53

7.2.3 Inductance. Neumann Formula for the Mutual Inductance. Important Things about Mutual Inductance

10 Statistical Distributions Solutions

= ΔW a b. U 1 r m 1 + K 2

Electric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin

Energy Dissipation Gravitational Potential Energy Power

dx was area under f ( x ) if ( ) 0

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.

Unit 6. Magnetic forces

Data Structures. Element Uniqueness Problem. Hash Tables. Example. Hash Tables. Dana Shapira. 19 x 1. ) h(x 4. ) h(x 2. ) h(x 3. h(x 1. x 4. x 2.

Problem Set 3 SOLUTIONS

CHAPTER 2 ELECTROSTATIC POTENTIAL

Week 8. Topic 2 Properties of Logarithms

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information

EXPANSION OF LIQUIDS

FI 2201 Electromagnetism

SURFACE TENSION. e-edge Education Classes 1 of 7 website: , ,

Course Updates. Reminders: 1) Assignment #8 available. 2) Chapter 28 this week.

3.1 Magnetic Fields. Oersted and Ampere

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by

That is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton.

Chapter 6 Electrostatic Boundary Value Problems. Dr. Talal Skaik

( ) D x ( s) if r s (3) ( ) (6) ( r) = d dr D x

Chapter 6 Frequency Response & System Concepts

Previously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : ,

DIRECT CURRENT CIRCUITS

Physics 111. Uniform circular motion. Ch 6. v = constant. v constant. Wednesday, 8-9 pm in NSC 128/119 Sunday, 6:30-8 pm in CCLIR 468

Homework Assignment 5 Solution Set

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

SPH4UI 28/02/2011. Total energy = K + U is constant! Electric Potential Mr. Burns. GMm

( )( )( ) ( ) + ( ) ( ) ( )

Mark Scheme (Results) January 2008

9.4 The response of equilibrium to temperature (continued)

Sensors and Actuators Introduction to sensors

Homework Assignment 3 Solution Set

Physics Jonathan Dowling. Lecture 9 FIRST MIDTERM REVIEW

MAGNETIC EFFECT OF CURRENT & MAGNETISM

A, Electromagnetic Fields Final Exam December 14, 2001 Solution

Chapter 22 The Electric Field II: Continuous Charge Distributions

PHYSICS 102. Intro PHYSICS-ELECTROMAGNETISM

Physics 1502: Lecture 2 Today s Agenda

Exam 1 September 21, 2012 Instructor: Timothy Martin

NS-IBTS indices calculation procedure

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

Physics 122, Fall December 2012

Transcription:

Ch 26 - Cpcitnce! Wht s Next! Cpcitnce" One week unit tht hs oth theoeticl n pcticl pplictions! Cuent & Resistnce" Moving chges, finlly!! Diect Cuent Cicuits! Pcticl pplictions of ll the stuff tht we ve een tlking out! "Electicl Btteyf Leyen js, meicn Philosophicl Society, Photo Ceit: Pete Hholt Review! 1.) 3.) L this week! q1q2 2 F E q0 Fk Electic Fiels " Exist in the pesence of chge pticles, pply foces to othe chges! q Guss s Lw!! # E in "0 Cn e use to etemine electic fiel in cetin situtions! U! " F! " qe Electic Enegy" Mesue of how much wok it tkes to q V!k move chges though electic fiels! Electic Potentil" V! " E s Mesue of how much enegy pe unit V chge it tkes to move though fiels! E! 2.) 4.)

Cpcitnce! Cpcitnce the ility to stoe chge.! C! Q "V [ Couloms] Volts [ ]! [ Fs] Cpcitnce is lwys positive, n is mesue of how much chge cn e stoe t given electic potentil.! 5.) Exmple 2! 2 conucting pltes hve chge of 1.2mC on ech, with 6.00-V potentil iffeence etween the two of them. Wht is the cpcitnce of this system?! +Q -Q 2.0x10!4 fs 7.) Exmple 1! Wht is the cpcitnce of this system, whee ech conucto hs chge of +/- 3 Couloms, n 9- Volt potentil exists etween the two conuctos?! Demo 1! Pllel Plte Cpcito! Physlet I. 26.1 1/3 F 6.) 8.)

Theoeticl Cpcitnce! Clculte the cpcitnce of n isolte conucto with chge Q n ius R. (ssume tht secon, concentic, hollow conucto exists with.)! if V k Q (fo this sphee) we cn wite: C Q V Q! k Q $ " # % & Exmple 3 - Pllel Plte Cpcito! Consie two pllel pltes, ech with e, septe y istnce n with equl n opposite chges on them. ssume tht pltes e close togethe compe to thei e so tht we cn neglect the ege effects n ssume tht E is constnt etween them. Clculte the cpcitnce of this system.! +Q -Q k 4'( o 9.) 11.) Sttegy! We cn clculte the cpcitnce of othe types of systems, using this sic sttegy:! 1. ssume chge of mgnitue Q! 2. Clculte V etween the pltes (using techniques fom lst chpte)! 3. Use CQ/ V to evlute the cpcitnce! +Q -Q l Exmple 3 - Pllel Plte Cpcito! Note tht V cp!"v pltes! E! (etween pllel pltes) n E cn e eive using Guss's Lw n E q in. Becuse # o ll of the chge is on the insie of the plte:! E q in # E $ # E $ Q We know tht % V cp &V % E!! ' Q * ( ) +, # C Q V cp Q ' Q * ( ) +, "$ ( ) +Q -Q 10.) 12.)

Demo 2! Pllel-Plte Cpcito! Physlet I.26.2 Exmple 4 - Cylinicl Cp.! cylinicl conucto of ius n chge Q is coxil with lge cylinicl shell of ius n chge -Q. Fin the cpcitnce of the system if its length is l.! l 13.) E 2k! (evelope using Guss's Lw) "V cp V " V " E $ V c # 2k! % $ V c 2k! ln ( & ' ) * $ C Q l V c 2k ln # ( ) 15.) Demo 3--Dielectic-Fille Cpcito! When you plce n insulting mteil etween the pltes of cpcito, the insulto expeiences Vn e Wl effect tht genetes n inuce chge on the insulto s sufce. This pouces n electic fiel in the iection opposite the iection of the fiel genete y the chge on the cpcito s pltes. This, in tun, iminishes the voltge coss the pltes n, s consequence, the tio Q/V (i.e., the cpcito s cpcitnce) goes UP. Dielectics o thee things:.) They incese the cpcitnce of cpcito vi the mechnism expline ove;.) They llow the pltes of the cpcito to e vey close (theey incesing the cpcitnce of the cpcito); c.) They llow pltes of vey lge e (hence lge cpcitnce) to e olle up into vey smll cylinicl elements Exmple 5 - Spheicl Cp.! Detemine the cpcitnce of spheicl cpcito, with n inne sphee of ius chge to +Q, n n oute sphee of ius chge to -Q.! E kq (evelope using Guss's Lw) 2 V cp V! V! E " # V c kq " 2 $ # V c kq! ' % & ( ) # C Q V c k(! ) 14.) 16.)

The Electic Bttey! 1780s - Glvni vs. Volt! Chging Cpcito! If 9V ttey is connecte to 300 µf cpcito, how much chge uils up on the pltes?! Cloth o ppe soke in slt o ci. g (silve) Zn (zinc) 17.) 19.) How It Woks! Two electoes (con n zinc) e immese in ilute ci (the electolyte).! Chging Cpcito! If 9V ttey is connecte to 300 µf cpcito, how much chge uils up on the pltes?! C Zn Becuse Q is ll locte on one sie of plte (why?): E! E! Q #V C $V # E!! % Q ( & ' ) * + C Q Q " o V C Q ( ) 18.) 20.)

C effective C 1 + C 2 21.) Cpcitos in Pllel! Cpcitos with oth of thei ens connecte s shown e si to e connecte in pllel.! C 2 C 1 Cpcitos stoe Enegy! cpcito cn stoe chge, n then ischge though evice, oing Wok.! But how much Wok?! V 23.) Cpcitos in Seies! Cpcitos connecte in ow s shown e si to e connecte in seies.! C 1 C 2 Enegy Deivtion! Wht is the iffeentil wok equie to move iffeentil chge q fom one plte to the othe?! W Vq W q C q V W Q! 0 q C q W Q2 2C 1 C effective 1 C 1 + 1 C 2 22.) 24.)

Othe enegy fomule! U 1 2 Q 2 C 1 2 CV 2 1 2 QV Exmple 6! Exmine the cicuit hee, whee C 1 > C 2 n oth hve een chge to the sme potentil V.!.) Wht is the potentil etween points n efoe the switches e close?! V Q 1 C 1 +Q 1 -Q 1 C 1 C 2 -Q 2 +Q 2.) Wht hppens to chges fte the switches e close?! Chge enges itself until the voltge coss ech cpcito is the sme. s Q1 is gete thn Q2, Q1 s excess flows to Q2 until V1V2.! 25.) 27.) Exmple 6! Exmine the cicuit hee, whee C 1 > C 2 n oth hve een chge to the sme potentil V.! +Q 1 -Q 1 C 1 C 2 -Q 2 +Q 2. Wht is the potentil etween points n efoe the switches e close?". Wht hppens to chges fte the switches e close?" c. Wht is the potentil fom to long time fte the switches hve een close?". Wht is the enegy stoe in the system efoe n fte the closing of the switches?! Dielectics! n insulto insete etween the pltes of n isolte pllel-plte cpcito cuses ecese in the potentil iffeence etween the two pltes, ecese of fcto 1!.! Why? Wht effect oes this hve on cpcitnce of the system?! C o Q o V o V V o! C Q o V Q o V o /!! Q o V o C!C o 26.) 30.)

Dielectic Vlues! Mteil!Dielectic!!Dielectic"!!Constnt (! )!!Stength (V/m)! Vcuum!1.00000!!------! i (y)!1.00059!!3e6! Ppe!!3.7!!!16e6! Wte!!80!!!------! C! o C! vntges to using ielectics in cpcitos inclue:! 1. incesing cpcitnce (!)! 2. incesing the mximum opeting voltge of the cpcito (most ielectics hve gete ekown stength thn i oes)! 3. the ielectic itself povies mechnicl suppot etween the pltes.! 31.) Exmple 7! pllel-plte cpcito hs pltes 2.0cm x 3.0 cm, septe only y 1.00mm thickness of ppe.!. Fin the evice s cpcitnce.!. Wht is the mximum chge tht cn e plce on the cpcito?! c. Wht is the mximum enegy tht cn e stoe in this cpcito?! 1. 19.7 pf 2. Dielectic stength16e6 V/m. VmxE16e6 0.001m)-16000V, so mx QCV(19.7pF)(16000V)0.315!C 3. UCV 2 /22.52e-3J 32.)