Copyright © 2009 Pearson Education, Inc. Admin: No assignment this week Discussion sections run as usual No labs in the week after spring break. Still.

Slides:



Advertisements
Similar presentations
Chapter 24 Capacitance, Dielectrics, Electric Energy Storage
Advertisements

Physics 2112 Unit 8: Capacitors
Unit 2 Day 3: Electric Energy Storage Electric potential energy stored between capacitor plates Work done to add charge to the capacitor plates Energy.
© 2012 Pearson Education, Inc. Which of the two arrangements shown has the smaller equivalent resistance between points a and b? Q26.1 A. the series arrangement.
Chapter 24 Capacitance, dielectrics and electric energy storage
Fall 2008Physics 231Lecture 4-1 Capacitance and Dielectrics.
Capacitance and Dielectrics
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Electric Potential Chapter 23 opener. We are used to voltage in our lives—a 12-volt car battery, 110 V or 220 V at home, 1.5 volt flashlight batteries,
Lecture 4 Capacitance and Capacitors Chapter 16.6  Outline Definition of Capacitance Simple Capacitors Combinations of Capacitors Capacitors with.
Chapter 23 Capacitance.
Lecture 8 Capacitance and capacitors
Application – Xerographic Copiers
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.
Tuesday, Oct. 4, 2011PHYS , Fall 2011 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #11 Tuesday, Oct. 4, 2011 Dr. Jaehoon Yu Capacitors in Series.
Bright Storm on Capacitors (Start to minute 7:10).
Objectives: 1. Define and calculate the capacitance of a capacitor. 2. Describe the factors affecting the capacitance of the capacitor. 3. Calculate the.
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.
(Capacitance and capacitors)
Review Lecture 2. Copyright © 2009 Pearson Education, Inc. Admin: Mid-term is in class on Wednesday. No assignment this week. Labs and discussion sessions.
Copyright © 2009 Pearson Education, Inc. Lecture 5 - Capacitance Capacitors & Dielectrics.
Dr. Jie ZouPHY Chapter 26 Capacitance and Dielectrics.
Capacitors Consider two large metal plates which are parallel to each other and separated by a distance small compared with their width. Area A The field.
Capacitance (II) Capacitors in circuits Electrostatic potential energy.
Chapter 24 Capacitance, Dielectrics, Electric Energy Storage
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. Admin: Discussion sections and Labs start this week. Do the pre-lab (2 points)!
Copyright © 2009 Pearson Education, Inc. May Term in Guatemala GDS 3559/STS 3500: Engineering Public Health: An Interdisciplinary Exploration of Community.
Capacitance and Dielectrics
 Devices that can store electric charge are called capacitors.  Capacitors consist of 2 conducting plates separated by a small distance containing an.
Copyright © 2009 Pearson Education, Inc. Various Capacitors Chapter 24 : Capacitance & Dielectrics. (in the book by Giancoli). Chapter 26 in our book.
Electric Potential. Electrostatic Potential Energy and Potential Difference The electrostatic force is conservative – potential energy can be defined.
Chapter 17 Electric Potential. Objectives: The students will be able to: Given the dimensions, distance between the plates, and the dielectric constant.
-Combinations of Capacitors -Energy Stored in a Charged Capacitor AP Physics C Mrs. Coyle.
Monday, Sept. 26, 2005PHYS , Fall 2005 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #8 Monday, Sept. 26, 2005 Dr. Jaehoon Yu Capacitors Determination.
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.
P212c25: 1 Chapter 25: Capacitance and Dielectrics Capacitor: two conductors (separated by an insulator) usually oppositely charged a +Q b -Q V ab proportional.
GENERAL PHYSICS LECTURE Chapter 26 CAPACITANCE AND DIELECTRICS Nguyễn Thị Ngọc Nữ PhD: Nguyễn Thị Ngọc Nữ.
111/16/2015 ELECTRICITY AND MAGNETISM Phy 220 Chapter 4: Capacitors.
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.
Chapter 16 Electrical Energy AndCapacitance. General Physics Review - Electric Potential for a system of point charges.
Chapter 23 Electric Potential. Basics The potential due to an electric dipole is just the sum of the potentials due to each charge, and can be calculated.
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Physics 212 Lecture 8, Slide 1 Physics 212 Lecture 8 Today's Concept: Capacitors How does a capacitor behave in a circuit? More circuit examples.
Capacitors The capacitor is an element that continuously stores charge (energy), for later use over a period of time! In its simplest form, a capacitor.
Capacitance (II) Capacitors in circuits Electrostatic potential energy.
I Chapter 25 Electric Currents and Resistance. I Problem (II) A 0.50μF and a 0.80 μF capacitor are connected in series to a 9.0-V battery. Calculate.
Capacitance. Device that stores electric charge. Construction: A capacitor is two conducting plates separated by a finite distance Typically separated.
Chapter 13 Electric Energy and Capacitance. Electric Potential Energy The electrostatic force is a conservative force It is possible to define an electrical.
Capacitor Device that can store electric charge Two conducting objects are placed near one another but not touching Power source charges up the plates,
Capacitors A capacitor is a device that has the ability “capacity” to store electric charge and energy.
Wednesday, Sep. 20, PHYS Ian Howley PHYS 1444 – Section 003 Lecture #8 Thursday Sep. 20, 2012 Ian Howley Chapter 24 Capacitors and Capacitance.
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Chapter 24: Capacitance and Dielectrics
Capacitors in Series & Parallel
Example: a parallel plate capacitor has an area of 10 cm2 and plate separation 5 mm. 300 V is applied between its plates. If neoprene is inserted between.
Capacitance and Dielectrics
Capacitors in Series & Parallel
17.1 Electric potential Energy
Phys102 Lecture 7/8 Capacitors
PHYS 1444 – Section 002 Lecture #11
PHYS 1444 – Section 003 Lecture #8
PHYS 1444 – Section 002 Lecture #11
Chapter 18: Electrical Potential Energy
Capacitors Devices used to store charge.
Physics for Scientists and Engineers, with Modern Physics, 4th edition
Chapter 24 Capacitance, Dielectrics, Electric Energy Storage
Chapter 26 Problems Solving
Presentation transcript:

Copyright © 2009 Pearson Education, Inc. Admin: No assignment this week Discussion sections run as usual No labs in the week after spring break. Still grading the tests: solutions posted

Copyright © 2009 Pearson Education, Inc. Thevenin 3 solution

Copyright © 2009 Pearson Education, Inc. R TH =R N V TH =I N R TH I R = I IN (R EQ /R)

Copyright © 2009 Pearson Education, Inc Determination of Capacitance Example 24-1: Capacitor calculations. (a)Calculate the capacitance of a parallel-plate capacitor whose plates are 20 cm × 3.0 cm and are separated by a 1.0-mm air gap. (b) What is the charge on each plate if a 12-V battery is connected across the two plates? (c) What is the electric field between the plates? (d) Estimate the area of the plates needed to achieve a capacitance of 1 F, given the same air gap d.

Copyright © 2009 Pearson Education, Inc. Capacitors are now made with capacitances of 1 farad or more, but they are not parallel-plate capacitors. Instead, they are activated carbon, which acts as a capacitor on a very small scale. The capacitance of 0.1 g of activated carbon is about 1 farad. Some computer keyboards use capacitors; depressing the key changes the capacitance, which is detected in a circuit.

Copyright © 2009 Pearson Education, Inc. Charging a capacitor involves removing charge from one plate and adding it to the other. This takes energy – and it becomes more difficult as the charge on the plates builds up. (It also takes time – more on this later)

Copyright © 2009 Pearson Education, Inc. A charged capacitor stores electric energy; the energy stored is equal to the work done to charge the capacitor: work doneEnergy stored For a small charge, dq: For total charge, Q:

Copyright © 2009 Pearson Education, Inc Electric Energy Storage Example 24-8: Energy stored in a capacitor. A camera flash unit stores energy in a 150-μF capacitor at 200 V. (a) How much electric energy can be stored? (b) What is the power output if nearly all this energy is released in 1.0 ms?

Copyright © 2009 Pearson Education, Inc Electric Energy Storage Conceptual Example 24-9: Capacitor plate separation increased. A parallel-plate capacitor carries charge Q and is then disconnected from a battery. The two plates are initially separated by a distance d. Suppose the plates are pulled apart until the separation is 2d. How has the energy stored in this capacitor changed?

Copyright © 2009 Pearson Education, Inc. Capacitors in parallel have the same voltage across each one. The equivalent capacitor is one that stores the same charge when connected to the same battery: 24-3 Capacitors in Series and Parallel Capacitors in parallel add like resistors in series The Capacitance increases.

Copyright © 2009 Pearson Education, Inc. Capacitors in series have the same charge. In this case, the equivalent capacitor has the same charge across the total voltage drop. Note that the formula is for the inverse of the capacitance and not the capacitance itself! 24-3 Capacitors in Series and Parallel Capacitors in series add like resistors in parallel. C eq gets smaller (smaller than the smallest individual capacitor)

Copyright © 2009 Pearson Education, Inc. The math In parallel, the voltage across each capacitor is the same, so: Q 1 + Q 2 + Q 3 = Q = VC 1 +VC 2 +VC 3 So Q=V(C 1 +C 2 +C 3 ) and Q=VC eq In series, the charge across each capacitor is the same, so: V = V 1 +V 2 +V 3 And Q/C eq = Q/C 1 + Q/C 2 + Q/C 3 So:

Copyright © 2009 Pearson Education, Inc Capacitors in Series and Parallel Example 24-5: Equivalent capacitance. Determine the capacitance of a single capacitor that will have the same effect as the combination shown.