EMF 2005 Handout 5: Capacitance 1 CAPACITANCE. Q Coulombs. Volts

Similar documents
Capacitance. Applications of Electric Potential. Capacitors in Kodak Cameras 3/17/2014. AP Physics B

Potential and Capacitance

ELECTROSTATIC FIELDS IN MATERIAL MEDIA

Chapter 6. Dielectrics and Capacitance

UNIT 4:Capacitors and Dielectric

Phys102 Second Major-102 Zero Version Coordinator: Al-Shukri Thursday, May 05, 2011 Page: 1

Where A is the plate area and d is the plate separation.

Chapter 2 GAUSS LAW Recommended Problems:

Q1. In figure 1, Q = 60 µc, q = 20 µc, a = 3.0 m, and b = 4.0 m. Calculate the total electric force on q due to the other 2 charges.

Physics 102. Second Midterm Examination. Summer Term ( ) (Fundamental constants) (Coulomb constant)

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

clicker 1/25/2011 All C s are 8.00 nf. The battery is 12 V. What is the equivalent capacitance? summary o

Chapter 16. Capacitance. Capacitance, cont. Parallel-Plate Capacitor, Example 1/20/2011. Electric Energy and Capacitance

( ) Energy storage in CAPACITORs. q C

STUDENT NAME: STUDENT id #: WORK ONLY 5 QUESTIONS


( ) ( ) ( ) ( ) ( z) ( )

CHAPTER: 2 ELECTROSTATIC POTENTIAL AND CAPACITANCE

Edexcel GCSE Physics

GAUSS' LAW E. A. surface

Capacitance. PHY2049: Chapter 25 1

Energy considerations Energy considerations

Chapter 19. Electric Potential Energy and the Electric Potential

Goal of this chapter is to learn what is Capacitance, its role in electronic circuit, and the role of dielectrics.

TOPPER SAMPLE PAPER 2 Class XII- Physics

Chapter 24: Capacitance and Dielectrics

Physics for Scientists & Engineers 2

PHYS 221 General Physics II

Electricity & Optics

Experiment #4 Gauss s Law Prelab Hints

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

Electric Current and Resistance

Q1. A) 48 m/s B) 17 m/s C) 22 m/s D) 66 m/s E) 53 m/s. Ans: = 84.0 Q2.

BASIC DIRECT-CURRENT MEASUREMENTS

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.

Electrostatics: Capacitor Examples

Thermodynamics and Equilibrium

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

Phys102 Final-061 Zero Version Coordinator: Nasser Wednesday, January 24, 2007 Page: 1

PHY 2054C Review guide Fall 2018 Chapter 17 Wave optics

ALUMINIUM ELECTROLYTIC CAPACITORS PG - LL9 Long Life Grade

Plan o o. I(t) Divide problem into sub-problems Modify schematic and coordinate system (if needed) Write general equations

Chapter 24 Capacitance and Dielectrics

MAGNETIC FIELDS CURRENT & RESISTANCE

CHAPTER 24 GAUSS LAW

" E ds = 0 becomes " E ds = 0 # d$ B. ! Not only charges produce E-field. ! a changing B-field also produces an E-field.

V q.. REASONING The potential V created by a point charge q at a spot that is located at a

5-4 Electrostatic Boundary Value Problems

**DO NOT ONLY RELY ON THIS STUDY GUIDE!!!**

PHYS 219 Spring semester Lecture 02: Coulomb s Law how point charges interact. Ron Reifenberger Birck Nanotechnology Center Purdue University

Schedule. Time Varying electromagnetic fields (1 Week) 6.1 Overview 6.2 Faraday s law (6.2.1 only) 6.3 Maxwell s equations

Chapter 19. Electrochemistry. Dr. Al Saadi. Electrochemistry

Sodium D-line doublet. Lectures 5-6: Magnetic dipole moments. Orbital magnetic dipole moments. Orbital magnetic dipole moments

General Physics II. Conducting concentric spheres Two concentric spheres of radii R and r. The potential difference between the spheres is

Synchronous Motor V-Curves

Hooke s Law (Springs) DAVISSON. F A Deformed. F S is the spring force, in newtons (N) k is the spring constant, in N/m

Physical Nature of the Covalent Bond Appendix H + H > H 2 ( ) ( )

Chapter 14 GAUSS'S LAW

Exam #2, Electrostatics

Transduction Based on Changes in the Energy Stored in an Electrical Field

Today in Physics 122: capacitors

Can current flow in electric shock?

Coulomb = V m. The line integral of the electric field around any closed path is always zero (conservative field)

Fri. 10/23 (C14) Linear Dielectrics (read rest at your discretion) Mon. (C 17) , E to B; Lorentz Force Law: fields

= (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

11. DUAL NATURE OF RADIATION AND MATTER

Second Major Solution Q1. The three capacitors in the figure have an equivalent capacitance of 2.77 µf. What is C 2?

Chapter 3. Electric Flux Density, Gauss s Law and Divergence

Lab 11 LRC Circuits, Damped Forced Harmonic Motion

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

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string?

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

Section 5.8 Notes Page Exponential Growth and Decay Models; Newton s Law

AQA GCSE Physics. Topic 7: Magnetism and Electromagnetism. Notes. (Content in bold is for Higher Tier only)

Chapter VII Electrodynamics

Chapter 26 - Capacitance

Supplementary Course Notes Adding and Subtracting AC Voltages and Currents

Chapter 2: Capacitor And Dielectrics

Electric Charge. Electric charge is quantized. Electric charge is conserved

Module 4: General Formulation of Electric Circuit Theory

Chapters 29 and 35 Thermochemistry and Chemical Thermodynamics

Where C is proportionally constant called capacitance of the conductor.

Get Solution of These Packages & Learn by Video Tutorials on

W V. (d) W. (3) Which one is used to determine the internal resistance of a cell

AQA GCSE Physics. Topic 4: Atomic Structure. Notes. (Content in bold is for Higher Tier only)

Sections 15.1 to 15.12, 16.1 and 16.2 of the textbook (Robbins-Miller) cover the materials required for this topic.

1. Transformer A transformer is used to obtain the approximate output voltage of the power supply. The output of the transformer is still AC.

Honors Physics Final Review Summary

Lecture 02 CSE 40547/60547 Computing at the Nanoscale

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review

Chemistry 20 Lesson 11 Electronegativity, Polarity and Shapes

Dielectrics 9.1 INTRODUCTION 9.2 DIELECTRIC CONSTANT

Solution to Quiz 2. April 18, 2010

Lecture 5: Equilibrium and Oscillations

Lecture 6: Phase Space and Damped Oscillations

Chapter 2. Coulomb s Law and Electric Field Intensity

Phy 212: General Physics II 1 Chapter 18 Worksheet 3/20/2008

Lecture 4. Electric Potential

General Chemistry II, Unit I: Study Guide (part I)

Class 6 : Insulating Materials

Transcription:

MF 005 Hanut 5: apacitance APAITAN Definitin f capacitance Recall: Fr a pint charge r a charge sphere V 4πε r In general, POTNTIAL HARG fr any size r shape f cnuctr. Definitin: The cnstant f prprtinality between V an is calle APAITAN, : V Units f capacitance: ulmbs Vlts V Definitin: Fara (F) V apacitance is a measure f the ability f a cnuctr r a system f cnuctrs t stre charge (an hence t stre energy). Recall: Fr a charge cnuctr U tt V U tt V r U tt Relatinship between capacitance an energy Alternative units fr ε : ulmbs 4πε r ε metres Vlts metres ε ulmbs (Vlts)(metres) Faras metres ε Fm These are the units in which ε is usually qute.

MF 005 Hanut 5: apacitance Prceure fr fining capacitance. Imagine a charge n the cnuctr (if it s a single cnuctr) r charges f ± (fr a pair f cnuctrs). Fin (e.g., use Gauss s Law) 3. Fin the ptential (ifference) using V L (never min the sign). 4. Put /V [ always cancels ut] a b Nte:. epens nly n the gemetry the size an shape f the cnuctrs an the istance between them.. is inepenent f [because V ] xamples:. apacitance f an islate sphere. Parallel plate capacitr 3. apacitance f tw cncentric spheres 4. apacitance per unit length f a caxial cable See lecture ntes

MF 005 Hanut 5: apacitance 3 apacitr An electrical cmpnent esigne t have a particular value f. apacitrs in parallel is the same fr bth: tt tt tt tt tt tt Therefre tt tt V apacitrs in series tt tt In this case is the same fr bth an is ifferent. V V tt tt tt tt tt

MF 005 Hanut 5: apacitance 4 Dielectrics an plarisatin Until nw, we have assume that the space between charges, cnuctrs, etc. is empty (a vacuum). What if it s fille with sme insulating material? Recall: A DILTRI (insulatr) is electrically neutral. But it cntains many ve an ve charges in its atms r mlecules. Because it s an insulatr, the charges can t mve arun. BUT: sme mlecules have a natural DIPOL MOMNT when place in an external electric fiel, the iples ten t align with it. iple Trque ven if n INTRINSI iples exist, they can be INDUD by an applie fiel, prucing the same effect. nsier a parallel plate capacitr, with psitive an negative charges n the plates. This creates an electric fiel between the plates. If there is a ielectric between the plates, then ue t iple alignment, r (POLARISATION) the istributins f ve an ve charge nt verlap exactly: xcess ve charge n the right. xcess ve charge n the left. The inuce (POLARISD) fiel, i, tens t OPPOS. The resultant fiel is LSS than the applie fiel: tt i i

MF 005 Hanut 5: apacitance 5 Dielectric cnstant tt i Let tt (K ) K K (smetimes written as the greek letter κ kappa) is the DILTRI ONSTANT r RLATIV PRMITTIVITY f the material. Let σ charge ensity n capacitr plates: Let σ i inuce charge ensity n surfaces f ielectric: σ /ε i σ i /ε Therefre σ ε ε [ ] i i tt ε K S the inuce surface charge ensity is σ i σ K The effect f ielectric cnstant n capacitance nsier the case f a parallel plate capacitr. N ielectric: εa With ielectric: K KεA apacitance with ielectric K( apacitance withut ielectric) S, capacitance (i.e., the ability t stre charge an hence energy) is increase by the use f a ielectric.

MF 005 Hanut 5: apacitance 6 Typical values f ielectic cnstant K Air.00059 (nt much ifferent frm a vacuum) Plythene.3 Glass 5 0 Germanium 6 Water 80 A perfect cnuctr? Gauss's Law in ielectrics Just replace ε with Kε : Φ A Kε enclse Dielectric breakwn If > sme limit, the BRAKDOWN FILD STRNGTH f the material, then the bns between the electrns an the atms are brken an the material becmes a ONDUTOR ( shrt circuit in a cable r capacitr).

MF 005 Hanut 5: apacitance 7 apacitance per unit length f a pair f caxial cyliners (e.g., a caxial cable) a b Step : Let charge per unit length be λ n inner cnuctr λ n uter cnuctr Step : Fin : Fiel pattern: Fiel lines g frm ve charges n inner cnuctr t ve charges n uter cnuctr 0 fr r < a an r > b (A Gaussian cyliner enclses n charge) λ Apply Gauss s Law πεr (similar t a previus example) Step 3: Fin : L Path: Integrate alng a fiel line L an L is parallel t s L r b λ λ b r ln πε r πε a a r r b L r a r 0 We take t be psitive when fining capacitance. Step 4: Put /V πε (apacitance/unit length) b ln a