111/16/2015 ELECTRICITY AND MAGNETISM Phy 220 Chapter 4: Capacitors.

Slides:



Advertisements
Similar presentations
before the plates were pulled apart.
Advertisements

Chapter 24 Capacitance, Dielectrics, Electric Energy Storage
Chapter 23: Electrostatic Energy and Capacitance
Chapter 24 Capacitance, dielectrics and electric energy storage
Fall 2008Physics 231Lecture 4-1 Capacitance and Dielectrics.
Capacitance and Dielectrics
Lecture 4 Capacitance and Capacitors Chapter 16.6  Outline Definition of Capacitance Simple Capacitors Combinations of Capacitors Capacitors with.
Chapter 23 Capacitance.
Capacitance and Dielectrics
Lecture 8 Capacitance and capacitors
Application – Xerographic Copiers
15/20/2015 General Physics (PHY 2140) Lecture 6  Electrostatics and electrodynamics Capacitance and capacitors capacitors with dielectrics Electric current.
17-7 Capacitance A device that stores electric charge Two plates that are separated by an insulator Used in electronic circuits Store charge that can later.
February 16, 2010 Potential Difference and Electric Potential.
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.
Capacitance and Dielectrics
ELECTRICITY PHY1013S CAPACITANCE Gregor Leigh
Bright Storm on Capacitors (Start to minute 7:10).
1 Capacitance and Dielectrics Chapter 27 Physics chapter 27.
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.
Dr. Jie ZouPHY Chapter 26 Capacitance and Dielectrics.
Capacitance and Dielectrics
Chapter 26 Capacitance and Dielectrics. Concept Question 1.
Capacitance & Dielectrics
FCI1 CHAPTER OUTLINE 1. Definition of Capacitance 2. Calculating Capacitance 3. Combinations of Capacitors 4. Energy Stored in a Charged Capacitor.
Copyright © 2009 Pearson Education, Inc. May Term in Guatemala GDS 3559/STS 3500: Engineering Public Health: An Interdisciplinary Exploration of Community.
Lecture 10 Capacitance and capacitors
Capacitance�and�Dielectrics
Capacitance and Dielectrics
Electrical Energy and Capacitance
 Devices that can store electric charge are called capacitors.  Capacitors consist of 2 conducting plates separated by a small distance containing an.
Capacitance.
Capacitance and Dielectrics
Chapter 17 Electric Potential. Objectives: The students will be able to: Given the dimensions, distance between the plates, and the dielectric constant.
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.
Electric Energy and Capacitance
P212c25: 1 Chapter 25: Capacitance and Dielectrics Capacitor: two conductors (separated by an insulator) usually oppositely charged a +Q b -Q V ab proportional.
110/24/2015 Applied Physics Lecture 5  Electrostatics Electrical energy potential difference and electric potential potential energy of charged conductors.
GENERAL PHYSICS LECTURE Chapter 26 CAPACITANCE AND DIELECTRICS Nguyễn Thị Ngọc Nữ PhD: Nguyễn Thị Ngọc Nữ.
CHAPTER 17 CAPACITOR & DIELECTRICS (PST :3 hours) (PDT : 7 hours)
Electrical Capacitance:
Physics 1202: Lecture 5 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
Monday, Feb. 13, 2006PHYS , Spring 2006 Dr. Jaehoon Yu 1 PHYS 1444 – Section 501 Lecture #8 Monday, Feb. 13, 2006 Dr. Jaehoon Yu Capacitors and.
Capacitance. Characteristics of a Capacitor No Dielectric Uniform Electric Field d Area Note: Net charge of the system.
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.
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Today’s agenda: Capacitance. You must be able to apply the equation C=Q/V. Capacitors: parallel plate, cylindrical, spherical. You must be able to calculate.
Capacitor Engr. Faheemullah Shaikh Lecturer, Department of Electrical Engineering.
Physics 2102 Jonathan Dowling Physics 2102 Lecture 8 Capacitors II.
12/4/2016 Advanced Physics Capacitance  Chapter 25 – Problems 1, 3, 8, (17), 19, (33), 39, 40 & 49.
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.
Wednesday, Sep. 20, PHYS Ian Howley PHYS 1444 – Section 003 Lecture #8 Thursday Sep. 20, 2012 Ian Howley Chapter 24 Capacitors and Capacitance.
Chapter 24: Capacitance and Dielectrics
Electric Energy and Capacitance
Capacitance and Dielectrics
Capacitors: parallel plate, cylindrical, spherical.
General Physics (PHY 2140) Lecture 5 Electrostatics Electrical energy
Introduction to Capacitance
General Physics (PHY 2140) Lecture 3 Electrostatics Electrical energy
General Physics (PHY 2140) Lecture 6 Electrostatics
Capacitor A device that stores energy by maintaining a separation between positive and negative charge. Can store electric charge / energy in the electric.
Consider two conductors carrying charges of equal magnitude but of opposite sign, Such a combination of two conductors is called a capacitor. The capacitance.
Capacitor Is a device that stores energy by maintaining a separation between positive and negative charge. Compare stored energy / charge to a bucket.
Presentation transcript:

111/16/2015 ELECTRICITY AND MAGNETISM Phy 220 Chapter 4: Capacitors

211/16/2015 a +Q b -Q 4.1 The definition of capacitance Capacitor: two conductors (separated by an insulator) usually oppositely charged The capacitance, C, of a capacitor is defined as a ratio of the magnitude of a charge on either conductor to the magnitude of the potential difference between the conductors

311/16/ A capacitor is basically two parallel conducting plates with insulating material in between. The capacitor doesn’t have to look like metal plates. 2.When a capacitor is connected to an external potential, charges flow onto the plates and create a potential difference between the plates. 3.Capacitors in circuits symbols: 4.Analysis follow from conservation of energy and conservation of charge Capacitor for use in high-performance audio systems

411/16/2015 Units of capacitance The unit of C is the farad (F), but most capacitors have values of C ranging from picofarads to microfarads (pF to  F). Recall, micro  10 -6, nano  10 -9, pico  If the external potential is disconnected, charges remain on the plates, so capacitors are good for storing charge (and energy).

511/16/2015 A A +Q -Q d 4.2 The parallel-plate capacitor The capacitance of a device depends on the geometric arrangement of the conductors where A is the area of one of the plates, d is the separation,  0 is a constant called the permittivity of free space,  0 = 8.85  C 2 /N·m 2  0 = 8.85  C 2 /N·m 2

611/16/2015 Proof: According to example 2.4.3,chapter 2, the value of the electric field between the plates is Because the field between the plates is uniform, the magnitude of the potential difference between the plates equals Ed, Because the field between the plates is uniform, the magnitude of the potential difference between the plates equals Ed, therefore, So we find that the capacitance is

711/16/2015 A parallel plate capacitor has plates 2.00 m 2 in area, separated by a distance of 5.00 mm. A potential difference of 10,000 V is applied across the capacitor. Determine the capacitance the charge on each plate Problem: parallel-plate capacitor

811/16/2015 A parallel plate capacitor has plates 2.00 m 2 in area, separated by a distance of 5.00 mm. A potential difference of 10,000 V is applied across the capacitor. Determine the capacitance the charge on each plate Given:  V=10,000 V A = 2.00 m 2 d = 5.00 mm Find: C=? Q=? Solution: Since we are dealing with the parallel-plate capacitor, the capacitance can be found as Once the capacitance is known, the charge can be found from the definition of a capacitance via charge and potential difference:

911/16/ Combinations of capacitors It is very often that more than one capacitor is used in an electric circuit We would have to learn how to compute the equivalent capacitance of certain combinations of capacitors C1C1 C2C2 C3C3 C5C5 C1C1 C2C2 C3C3 C4C4

1011/16/2015 +Q 1 Q1Q1 C1C1 V=V ab a b +Q 2 Q2Q2 C2C2 a. Parallel combination Connecting a battery to the parallel combination of capacitors is equivalent to introducing the same potential difference for both capacitors, A total charge transferred to the system from the battery is the sum of charges of the two capacitors, By definition, Thus, C eq would be

1111/16/2015 Parallel combination: notes Analogous formula is true for any number of capacitors, It follows that the equivalent capacitance of a parallel combination of capacitors is greater than any of the individual capacitors (parallel combination)

1211/16/2015 A 3  F capacitor and a 6  F capacitor are connected in parallel across an 18 V battery. Determine the equivalent capacitance and total charge deposited. Problem: parallel combination of capacitors

1311/16/2015 A 3  F capacitor and a 6  F capacitor are connected in parallel across an 18 V battery. Determine the equivalent capacitance and total charge deposited. +Q 1 Q1Q1 C1C1 V=V ab a b +Q 2 Q2Q2 C2C2 Given: V = 18 V C 1 = 3  F C 2 = 6  F Find: C eq =? Q=? First determine equivalent capacitance of C 1 and C 2 : Next, determine the charge

1411/16/2015 b. Series combination Connecting a battery to the serial combination of capacitors is equivalent to introducing the same charge for both capacitors, A voltage induced in the system from the battery is the sum of potential differences across the individual capacitors, By definition, Thus, C eq would be +Q 1 Q1Q1 C1C1 +Q 2 Q2Q2 C2C2 V=V ab a c b

1511/16/2015 Series combination: notes Analogous formula is true for any number of capacitors, It follows that the equivalent capacitance of a series combination of capacitors is always less than any of the individual capacitance in the combination (series combination)

1611/16/2015 A 3  F capacitor and a 6  F capacitor are connected in series across an 18 V battery. Determine the equivalent capacitance. Problem: series combination of capacitors

1711/16/2015 A 3  F capacitor and a 6  F capacitor are connected in series across an 18 V battery. Determine the equivalent capacitance and total charge deposited. +Q 1 Q1Q1 C1C1 +Q 2 Q2Q2 C2C2 V=V ab a c b Given: V = 18 V C 1 = 3  F C 2 = 6  F Find: C eq =? Q=? First determine equivalent capacitance of C 1 and C 2 : Next, determine the charge

1811/16/ Energy stored in a charged capacitor The energy (U) stored on a capacitor is given by:

1911/16/2015   Find electric field energy density (energy per unit volume) in a parallel-plate capacitor Example: electric field energy in parallel-plate capacitor Recall Thus, and so, the energy density is

2011/16/2015 C1C1 C2C2 V C3C3 In the circuit shown V = 48V, C 1 = 9  F, C 2 = 4  F and C 3 = 8  F. (a)determine the equivalent capacitance of the circuit, (b) determine the energy stored in the combination by calculating the energy stored in the equivalent capacitance. Example: stored energy

2111/16/2015 C1C1 C2C2 V C3C3 In the circuit shown V = 48V, C 1 = 9  F, C 2 = 4  F and C 3 = 8  F. (a) determine the equivalent capacitance of the circuit, (b) determine the energy stored in the combination by calculating the energy stored in the equivalent capacitance, First determine equivalent capacitance of C 2 and C 3 : The energy stored in the capacitor C 123 is then Next, determine equivalent capacitance of the circuit by noting that C 1 and C 23 are connected in series Given: V = 48 V C 1 = 9  F C 2 = 4  F C 3 = 8  F Find: C eq =? U=?

2211/16/2015 QQ QQ QQ QQ V0V0 V 4.5 Capacitors with dielectrics A dielectrics is an insulating material (rubber, glass, etc.) Consider an insolated, charged capacitor Notice that the potential difference decreases (k = V 0 /V) Since charge stayed the same (Q=Q 0 ) → capacitance increases dielectric constant: k = C/C 0 Dielectric constant is a material property Insert a dielectric

2311/16/2015 Capacitors with dielectrics - notes Capacitance is multiplied by a factor k when the dielectric fills the region between the plates completely E.g., for a parallel-plate capacitor There exists a maximum of the electric field, sometimes called dielectric strength, that can be produced in the dielectric before it breaks down

2411/16/2015 Dielectric constants and dielectric strengths of various materials at room temperature Material Dielectric constant, k Dielectric strength (V/m) Vacuum Air  10 6 Water80-- Fused quartz  10 6

2511/16/2015 Take a parallel plate capacitor whose plates have an area of 2000 cm 2 and are separated by a distance of 1cm. The capacitor is charged to an initial voltage of 3 kV and then disconnected from the charging source. An insulating material is placed between the plates, completely filling the space, resulting in a decrease in the capacitors voltage to 1 kV. Determine the original and new capacitance, the charge on the capacitor, and the dielectric constant of the material. Example

2611/16/2015 Take a parallel plate capacitor whose plates have an area of 2 m 2 and are separated by a distance of 1cm. The capacitor is charged to an initial voltage of 3 kV and then disconnected from the charging source. An insulating material is placed between the plates, completely filling the space, resulting in a decrease in the capacitors voltage to 1 kV. Determine the original and new capacitance, the charge on the capacitor, and the dielectric constant of the material. Given:  V 1 =3,000 V  V 2 =1,000 V A = 2.00 m 2 d = 0.01 m Find: C=? C 0 =? Q=? k=? Since we are dealing with the parallel-plate capacitor, the original capacitance can be found as The charge on the capacitor can be found to be The dielectric constant and the new capacitance are