Capacitor: any two conductors, one with charge +Q, other with charge -Q Potential DIFFERENCE between conductors = V

Similar documents
Physics Lecture: 16 MON 23 FEB Capacitance I

Physics 2102 Gabriela González

Physics Jonathan Dowling. Physics 2102 Lecture 7 Capacitors I

Chapter 25. Capacitance

Physics (

Chapter 24 Capacitance and Dielectrics

Chapter 18. Circuit Elements, Independent Voltage Sources, and Capacitors

Can current flow in electric shock?

Capacitance and Dielectrics

Definition of Capacitance

Capacitance. Chapter 21 Chapter 25. K = C / C o V = V o / K. 1 / Ceq = 1 / C / C 2. Ceq = C 1 + C 2

Capacitors (Chapter 26)

shown in Fig. 4, is initially uncharged. How much energy is stored in the two capacitors after the switch S is closed for long time?

Friday July 11. Reminder Put Microphone On

Capacitors And Dielectrics

Chapter 24 Capacitance and Dielectrics

Chapter 26. Capacitance and Dielectrics

W05D1 Conductors and Insulators Capacitance & Capacitors Energy Stored in Capacitors

Physics Electricity & Op-cs Lecture 8 Chapter 24 sec Fall 2017 Semester Professor

Capacitance and Dielectrics. Chapter 26 HW: P: 10,18,21,29,33,48, 51,53,54,68

Reading: Electrostatics 3. Key concepts: Capacitance, energy storage, dielectrics, energy in the E-field.

Parallel Plate Capacitor, cont. Parallel Plate Capacitor, final. Capacitance Isolated Sphere. Capacitance Parallel Plates, cont.

Capacitance and capacitors. Dr. Loai Afana

F = Q big = c) The electric potential in a certain region of space can be described by the equation: 16y2 (1 + z 2 ) V (x, y, z) = 10x

Chapter 26. Capacitance and Dielectrics

University Physics (PHY 2326)

Today s agenda: Capacitors and Capacitance. You must be able to apply the equation C=Q/V.

Chapter 24: Capacitance and Dielectrics

Chapter 24 Capacitance and Dielectrics

EXAM REVIEW ON MONDAY

1. zero. Where an electric field line crosses an equipotential surface, the angle between the field line and the equipotential is

Chapter 24. Capacitance and Dielectrics Lecture 1. Dr. Armen Kocharian

PHYS 241 EXAM #1 October 5, 2006

Homework. Reading: Chap. 29, Chap. 31 and Chap. 32. Suggested exercises: 29.17, 29.19, 29.22, 29.23, 29.24, 29.26, 29.27, 29.29, 29.30, 29.31, 29.

Capacitance and Dielectrics

Phys222 W16 Exam 2: Chapters Key. Name:

Capacitance, Resistance, DC Circuits

Continuing our discussion on Capacitors

Physics 202, Exam 1 Review

Agenda for Today. Elements of Physics II. Capacitors Parallel-plate. Charging of capacitors

Consider a point P on the line joining the two charges, as shown in the given figure.

Electric Field of a uniformly Charged Thin Spherical Shell

Chapter 24 Capacitance, Dielectrics, Electric Energy Storage

Chapter 24: Capacitance and Dielectrics

F 13. The two forces are shown if Q 2 and Q 3 are connected, their charges are equal. F 12 = F 13 only choice A is possible. Ans: Q2.

Physics 212. Lecture 7. Conductors and Capacitance. Physics 212 Lecture 7, Slide 1

2014 F 2014 AI. 1. Why must electrostatic field at the surface of a charged conductor be normal to the surface at every point? Give reason.

which checks. capacitance is determined entirely by the dimensions of the cylinders.

Hollow Conductors. A point charge +Q is placed at the center of the conductors. The induced charges are: 1. Q(I1) = Q(I2) = -Q; Q(O1) = Q(O2)= +Q

Chapter 29. Electric Potential: Charged Conductor

PH213 Chapter 24 Solutions

Chapter 26. Capacitance and Dielectrics

Solution to Quiz 2. April 18, 2010

4) A 3.0 pf capacitor consists of two parallel plates that have surface charge densities of 1.0

Physics (

This work is licensed under a Creative Commons Attribution-Noncommercial-Share Alike 4.0 License.

= (series) Capacitors in series. C eq. Hence. Capacitors in parallel. Since C 1 C 2 V 1 -Q +Q -Q. Vab V 2. C 1 and C 2 are in series

AP Physics C - E & M. Slide 1 / 39 Slide 2 / 39. Slide 4 / 39. Slide 3 / 39. Slide 6 / 39. Slide 5 / 39. Capacitance and Dielectrics.

7. A capacitor has been charged by a D C source. What are the magnitude of conduction and displacement current, when it is fully charged?

Exam 1 Solutions. The ratio of forces is 1.0, as can be seen from Coulomb s law or Newton s third law.

iclicker A metal ball of radius R has a charge q. Charge is changed q -> - 2q. How does it s capacitance changed?

This work is licensed under a Creative Commons Attribution-Noncommercial-Share Alike 4.0 License.

CAPACITANCE Parallel-plates capacitor E + V 1 + V 2 - V 1 = + - E = A: Area of the plates. = E d V 1 - V 2. V = E d = Q =

PHYSICS - CLUTCH CH 24: CAPACITORS & DIELECTRICS.

4 pt. (in J) 3.A

Electric Potential Energy Conservative Force

Chapter 26. Capacitance and Dielectrics

INDIAN SCHOOL MUSCAT FIRST TERM EXAMINATION PHYSICS

Class 6. Capacitance and Capacitors. Physics 106. Winter Press CTRL-L to view as a slide show. Class 6. Physics 106.

Chapter 1 The Electric Force

AP Physics C. Electric Circuits III.C

Department of Physics. PHYS MAJOR 2 EXAM Test Code: 015. Monday 1 st May 2006 Exam Duration: 2hrs (from 6:30pm to 8:30pm)

Physics 196 Final Test Point

Louisiana State University Physics 2102, Exam 2, March 5th, 2009.

Agenda for Today. Elements of Physics II. Capacitors Parallel-plate. Charging of capacitors

Phys102 Second Major-181 Zero Version Coordinator: Kunwar, S Monday, November 19, 2018 Page: 1

Capacitance. PHY2049: Chapter 25 1

Review from yesterday. Please answer PROBLEM 3 in Knight on page 716 while we are waiting to start. It takes 3.0 μj to move a 15nC charge from A

Chapter 24: Capacitance and Dielectrics. Capacitor: two conductors (separated by an insulator) usually oppositely charged. (defines capacitance)

Look over. examples 1, 2, 3, 5, 6. Look over. Chapter 25 section 1-8. Chapter 19 section 5 Example 10, 11

Experiment FT1: Measurement of Dielectric Constant

CAPACITANCE: CHAPTER 24. ELECTROSTATIC ENERGY and CAPACITANCE. Capacitance and capacitors Storage of electrical energy. + Example: A charged spherical

Physics 219 Question 1 January

Physics 202, Exam 1 Review


Electric Potential Energy Chapter 16

(21/703) At what distance from a point charge of 8µC would the potential equal 3.6X10 4 V?

Chapter 24: Capacitance and Dielectrics

Sharpen thinking about connections among electric field, electric potential difference, potential energy

Physics Electricity and Magnetism Lecture 06 - Capacitance. Y&F Chapter 24 Sec. 1-6

Lecture 20. March 22/24 th, Capacitance (Part I) Chapter , Pages

13 - ELECTROSTATICS Page 1 ( Answers at the end of all questions )

Potential from a distribution of charges = 1

The Basic Capacitor. Dielectric. Conductors

LAST Name (print) ALL WORK MUST BE SHOWN FOR THE FREE RESPONSE QUESTION IN ORDER TO RECEIVE FULL CREDIT.

Q1. Three point charges are arranged as shown in FIGURE 1. Find the magnitude of the net electrostatic force on the point charge at the origin.

Which one of the pipes emits sound with the lowest frequency? Which one of the pipes emits sound with the next lowest frequency?

Question 1. The figure shows four pairs of charged particles. For each pair, let V = 0 at infinity and consider V net at points on the x axis.

Electric Potential. Capacitors (Chapters 28, 29)

C = V Q. To find the capacitance of two conductors:

Transcription:

Physics 2102 Gabriela González Capacitor: any two conductors, one with charge +Q, other with charge -Q Potential DIFFERENCE between conductors = V Units of capacitance: Farad (F) = Coulomb/Volt -Q +Q Uses: storing and releasing electric charge/energy. Most electronic capacitors: micro-farads (µf), pico-farads (pf) -- 10-12 F New technology: compact 1 F capacitors 1

Capacitance depends only on GEOMETRICAL factors and on the MATERIAL that separates the two conductors e.g. Area of conductors, separation, whether the space in between is filled with air, plastic, etc. +Q -Q (We first focus on capacitors where gap is filled by AIR!) Electrolytic (1940-70) Electrolytic (new) Paper (1940-70) Variable air, mica Tantalum (1980 on) Ceramic (1930 on) Mica (1930-50 2

Capacitor: any two conductors, one with charge +Q, other with charge Q Potential DIFFERENCE between conductors = V Units of capacitance: Farad (F) = Coulomb/Volt +Q -Q Uses: storing and releasing electric charge/energy. Most electronic capacitors: micro-farads (µf), pico-farads (pf) -- 10-12 F New technology: compact 1 F capacitors We want capacitance: C=Q/V E field between the plates: (Gauss Law) Area of each plate = A Separation = d charge/area = σ= Q/A Relate E to potential difference V: What is the capacitance C? +Q -Q 3

A huge parallel plate capacitor consists of two square metal plates of side 50 cm, separated by an air gap of 1 mm What is the capacitance? C = ε 0 A/d = (8.85 x 10-12 F/m)(0.25 m 2 )/(0.001 m) = 2.21 x 10-9 F (small!!) Lesson: difficult to get large values of capacitance without special tricks! C = Q V = Q Ed = ε 0 A d A parallel plate capacitor of capacitance C is charged using a battery. Charge = Q, potential difference = V. Battery is then disconnected. If the plate separation is INCREASED, does potential difference V: (a) Increase? (b) Remain the same? (c) Decrease? Q is fixed! C decreases (=ε 0 A/d) Q=CV; V increases. +Q -Q 4

C = Q V = Q Ed = ε 0A d A parallel plate capacitor of capacitance C is charged using a battery. Charge = Q, potential difference = V. Plate separation is INCREASED while battery remains connected. +Q -Q Does the electric field inside: (a) Increase? (b) Remain the same? (c) Decrease? V is fixed by battery! C decreases (=ε 0 A/d) Q=CV; Q decreases E = Q/ ε 0 A decreases What is the electric field inside the capacitor? (Gauss Law) Relate E to potential difference between the plates: Radius of outer plate = b Radius of inner plate = a Concentric spherical shells: Charge +Q on inner shell, -Q on outer shell 5

What is the capacitance? C = Q/V = Radius of outer plate = b Radius of inner plate = a Concentric spherical shells: Charge +Q on inner shell, -Q on outer shell Isolated sphere: let b >> a, What is the electric field in between the plates? Relate E to potential difference between the plates: Radius of outer plate = b Radius of inner plate = a Length of capacitor = L +Q on inner rod, -Q on outer shell cylindrical surface of radius r 6

What is the capacitance C? C = Q/V = Radius of outer plate = b Radius of inner plate = a Length of capacitor = L Charge +Q on inner rod, -Q on outer shell Example: co-axial cable. Any two charged conductors form a capacitor. Capacitance : C= Q/V Simple Capacitors: Parallel plates: C = ε 0 A/d Spherical : C = 4π ε 0 ab/(b-a) Cylindrical: C = 2π ε 0 L/ln(b/a) 7

A wire is a conductor, so it is an equipotential. Capacitors in parallel have SAME potential difference but NOT ALWAYS same charge. V AB = V CD = V Q total = Q 1 + Q 2 C eq V = C 1 V + C 2 V C eq = C 1 + C 2 Equivalent parallel capacitance = sum of capacitances A C Q 1 Q 2 C 1 C 2 B D PARALLEL: V is same for all capacitors Total charge in C eq = sum of charges Q total C eq Q 1 = Q 2 = Q (WHY??) V AC = V AB + V BC A Q 1 Q 2 B C C 1 C 2 Q SERIES: Q is same for all capacitors Total potential difference in C eq = sum of V C eq 8

In parallel : Q 1 C 1 C eq = C 1 + C 2 V eq =V 1 =V 2 Q eq =Q 1 +Q 2 Q 2 C 2 Q eq Ceq In series : Q 1 Q 2 1/C eq = 1/C 1 + 1/C 2 V eq =V 1 + V 2 Q eq =Q 1= Q 2 C 1 C 2 What is the charge on each capacitor? Q = CV; V = 120 V Q 1 = (10 µf)(120v) = 1200 µc Q 2 = (20 µf)(120v) = 2400 µc Q 3 = (30 µf)(120v) = 3600 µc Note that: Total charge (7200 µc) is shared between the 3 capacitors in the ratio C 1 :C 2 :C 3 -- i.e. 1:2:3 10 µf 20 µf 30 µf 120V 9

What is the potential difference across each capacitor? Q = CV; Q is same for all capacitors Combined C is given by: 10 µf 20 µf 30 µf C eq = 5.46 µf Q = CV = (5.46 µf)(120v) = 655 µc V 1 = Q/C 1 = (655 µc)/(10 µf) = 65.5 V V 2 = Q/C 2 = (655 µc)/(20 µf) = 32.75 V V 3 = Q/C 3 = (655 µc)/(30 µf) = 21.8 V 120V Note: 120V is shared in the ratio of INVERSE capacitances i.e.1:(1/2): (1/3) (largest C gets smallest V) In the circuit shown, what is the charge on the 10µF capacitor? The two 5µF capacitors are in parallel Replace by 10µF Then, we have two 10µF capacitors in series So, there is 5V across the 10µF capacitor of interest Hence, Q = (10µF )(5V) = 50µC 10 µf 10 µf 5 µf 5 µf 10V 10 µf 10V 10

Start out with uncharged capacitor Transfer small amount of charge dq from one plate to the other until charge on each plate has magnitude Q How much work was needed? dq Energy stored in capacitor:u = Q 2 /(2C) = CV 2 /2 View the energy as stored in ELECTRIC FIELD For example, parallel plate capacitor: Energy DENSITY = energy/volume = u = volume = Ad General expression for any region with vacuum (or air) 11

10µF capacitor is initially charged to 120V. 20µF capacitor is initially uncharged. Switch is closed, equilibrium is reached. How much energy is dissipated in the process? 10µF (C 1 ) Initial charge on 10µF = (10µF)(120V)= 1200µC 20µF (C 2 ) After switch is closed, let charges = Q 1 and Q 2. Charge is conserved: Q 1 + Q 2 = 1200µC Q 1 = 400µC Also, V final is same: Q 2 = 800µC V final = Q 1 /C 1 = 40 V Initial energy stored = (1/2)C 1 V initial 2 = (0.5)(10µF)(120) 2 = 72mJ Final energy stored = (1/2)(C 1 + C 2 )V final 2 = (0.5)(30µF)(40) 2 = 24mJ Energy lost (dissipated) = 48mJ DIELECTRIC +Q - Q C = κε 0 A/d If the space between capacitor plates is filled by a dielectric, the capacitance INCREASES by a factor κ This is a useful, working definition for dielectric constant. Typical values of κ: 10-200 12

Capacitor has charge Q, voltage V Battery remains connected while dielectric slab is inserted. Do the following increase, decrease or stay the same: Potential difference? Capacitance? Charge? Electric field? dielectric slab Initial values: capacitance = C; charge = Q; potential difference = V; electric field = E; Battery remains connected V is FIXED; V new = V (same) C new = κc (increases) Q new = (κc)v = κq (increases). Since V new = V, E new = E (same) dielectric slab Energy stored? u=ε 0 E 2 /2 => u=κε 0 E 2 /2 = εe 2 /2 13

Capacitors in series and in parallel: in series: charge is the same, potential adds, equivalent capacitance is given by 1/C=1/C 1 +1/C 2 in parallel: charge adds, potential is the same, equivalent capaciatnce is given by C=C 1 +C 2. Energy in a capacitor: U=Q 2 /2C=CV 2 /2; energy density u=ε 0 E 2 /2 Capacitor with a dielectric: capacitance increases C =κc 14