Today 2/28  Read Ch 19.3  Practice exam posted  Electric Potential Energy, PE E Electric Potential, V Electric Potential Difference,  V (watch out.

Slides:



Advertisements
Similar presentations
Day 15: Electric Potential due to Point Charges The Electric Potential of a Point Charge Work done to bring two point charges together The Electric Potential.
Advertisements

Physics 1161 Lecture 4 Potential & Potential Energy.
Electrical Energy and Electric Potential AP Physics C.
1 W03D2 Work, Potential Energy and Electric Potential Today’s Reading Assignment: Course Notes: Sections
When an object is dropped on earth, the work done by the gravitational force is equal to the change in gravitational potential energy: W = mgh initial.
Today 3/12  Plates if charge  E-Field  Potential  HW:“Plate Potential” Due Friday, 3/14.
Electric Potential. Gravitational Potential Energy B hBhB F = mg hAhA A GPE = mgΔh GPE = mgh A – mgh B GPE = Work (W) required to raise or lower the book.
1) Electric Charge I 1) one is positive, the other is negative 2) both are positive 3) both are negative 4) both are positive or both are negative Two.
Consider a point charge, +q fixed at the origin A positive test charge,q 0 is placed at A, a distance r A Coulomb’s law determines the magnitude of repulsive.
Physics 2113 Lecture 14: WED 18 FEB
Electric Potential Physics 102 Professor Lee Carkner Lecture 12.
Real Insulators (Dielectrics) If I bring a charged rod to a leaf electrometer: A] nothing will happen B] nothing will happen until I touch the electrometer.
Physics 6B Electric Potential and Electric Potential Energy Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Electric Potential Energy PH 203 Professor Lee Carkner Lecture 6.
General Physics II, Lec 7, By/ T.A. Eleyan 1 Additional Questions ( The Electric Potential )
Norah Ali Al-moneef king saud university
ConcepTest 2.1a Electric Potential Energy I
Electric Potential Physics 102 Professor Lee Carkner Lecture 12.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Physics 2102 Lecture 5 Electric Potential I Physics 2102
Electrical Energy and Electric Potential
Chapter 23 Electric Potential
Lecture 3 Electrical Energy Chapter 16.1  16.5 Outline Potential Difference Electric Potential Equipotential Surface.
Chapter 17 Electric Potential Energy and the Electric Potential.
Electric Potential, Electric Energy and Capacitance
Electric Potential and Electric Energy Chapter 17.
Electric Potential and Capacitance What’s a volt anyway? Presentation 2001 Dr. Phil Dauber as modified by R. McDermott.
Electrical Energy and Potential IB Physics. Electric Fields and WORK In order to bring two like charges near each other work must be done. In order to.
Voltage and Capacitance Chapter 29. Electric Potential Energy Potential Energy of a charge Wants to move when it has high PE Point b –U = max –K = min.
Electric Potential, Electric Potential Energy, and the Generalized Work Energy Theorem.
Physics 2112 Unit 5: Electric Potential Energy
Electric Potential A PowerPoint Presentation by
The Electric Potential
Electric Potential Energy and Potential 235 U nucleus + n (92 protons) BaKr (56 p) (36 p) d = m A B q 0 E.
Electric Potential Energy of the System of Charges
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Electrostatic Forces Homework: Complete handout. Magnitude of Force According to Coulomb’s Law  The magnitude of force exerted on a charge by another.
Electric Potential II Physics 2102 Jonathan Dowling Physics 2102 Lecture: 09 MON 02 FEB Ch
Chapter 23 Electric Potential.
Today 3/3  Read Ch 19.4  Practice exam posted  Energy of Assembly  Calculating Velocities  HW:“Charge Assembly 2” Due Thursday  Lab: “Mapping Equipotential.
Chapter 16 Electrical Energy and Capacitance Conceptual Quiz Questions.
Electric Potential & Electric Potential Energy. Electric Potential Energy The electrostatic force is a conservative (=“path independent”) force The electrostatic.
AP Physics C Montwood High School R. Casao
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Electric energy (Electric Potential Energy) Electric potential Gravitation.
There will be a quiz next class period, Feb 1, covering Ch 22 and the beginning of Ch 23 (what we cover in class today)
 Assess. Statements due Monday, 10/20/14.
Introduction to Electricity Electric charges come in two varieties. We have named these positive and negative. To be mathematically consistent all of electricity.
Electrical Energy and Potential
Chapter 6 Motion of Charged Particles in Electric Fields.
Wednesday, Sep. 14, PHYS Dr. Andrew Brandt PHYS 1444 – Section 04 Lecture #5 Chapter 21: E-field examples Chapter 22: Gauss’ Law Examples.
Lecture3 Dr. lobna Mohamed Abou El-magd
A metal box with no net charge is placed in an initially uniform E field, as shown. What is the total charge on the inner surface ? Assume this surface.
Lecture 5 Dr. Lobna Mohamed Abou El-Magd The Electric Potential.
Electric Potential. Gravitational Potential Energy B hBhB F = mg hAhA A GPE = mgΔh GPE = mgh A – mgh B GPE = Work (W) required to raise or lower the book.
Phys 102 – Lecture 4 Electric potential energy & work.
Announcements  Homework for tomorrow… Ch. 28: CQ 1 & 3, Probs. 6 & : 2.2 x m CQ10: a) +b) -c) : 2.7 x C/m : E 1 = 900.
Electric Field.
CHAPTER-24 Electric Potential.
-Electric Potential Energy -Electric Potential AP Physics C Mrs. Coyle.
Electric Potential.
Agenda Today & Monday– Problems Ch Tuesday – lab 5 & Quiz Today –Charged Building Blocks Distributions Atomic Stability –Continuous Charge Distribution.
Today5/2  Questions?  E-Fields and Potential Difference (review)
Physics 212 Lecture 5, Slide 1 Physics 212 Lecture 5 Electric Potential Energy.
1 Chapter-3 (Electric Potential) Electric Potential: The electrical state for which flow of charge between two charged bodies takes place is called electric.
Oct. 4, From last time(s)… Work, energy, and (electric) potential Electric potential and charge Electric potential and electric field. Electric charges,
Electrical Energy Fields Or Fields of Dreams 2. An electric charge changes the space around it so that other charges… Feel an electrical force – Electrical.
Chapter 22 : Electric potential
A proton and an electron are in a constant electric field created by oppositely charged plates. You release the proton from the positive side and the.
Chapter 23 Electric Potential.
Presentation transcript:

Today 2/28  Read Ch 19.3  Practice exam posted  Electric Potential Energy, PE E Electric Potential, V Electric Potential Difference,  V (watch out foe +/- signs!!!)  More than one charge  HW:“Charge Assembly” Due Monday 3/5

Problem: Two identical point charges of 0.01g are placed 1m apart. The right-hand charge is released. Find its velocity when it is 10cm farther away. Two opposite point charges of 0.01g are placed 1m apart. The right-hand charge is released. Find its velocity when it is 10cm closer. v = 0 v = ?

Problem: Two identical point charges of mass of 0.01g are placed 1m apart. The right-hand charge is released. Find its velocity when it is 10cm farther away. Two opposite point charges of 0.01g are placed 1m apart. The right-hand charge is released. Find its velocity when it is 10cm closer. v = 0 v = ? E Field and Force are not the same everywhere so F net = ma requires calculus. Also need a system to handle direction. Energy buckets are the way!

Problem: Two identical point charges og mass.01g are placed 1m apart. The right-hand charge is released. Find its velocity when it is 10cm farther away. v = 0v = ? PE E KEPE E KE Initial PE at A? Initial KE at A? Final PE at B? (More or less than before?) Final KE at B? 0 Equals the PE lost!  PE A,B = -  KE A,B AB Subscripts tell us from A to B

“Potential Energy Difference” and “Potential Difference” Potential Energy Difference  PE A,B is the change in PE the particular charge feels when it is moved from one location to another. Potential Difference  V A,B is the change in PE a positive 1C charge would feel if it were moved from one location to another.  V A,B = Volts, and q = +1  C  PE A,B = +100J  V A,B = Volts, and q = +1  C  PE A,B = -100J

Which way does the E Field point?  PE A,B = +100J, and q = +1  C What is  V A,B ?  V A,B = 10 8 Volts  V A,B = Volts  PE A,B = +100J, and q = -1  C What is  V A,B ? AB Higher Potential E Fields point “downhill” with respect to potential difference E field Remember: From A to B!!!

What about Work, W A,B ?  PE A,B = +100J, and q = +1  C What is  V A,B ?  V A,B = 10 8 Volts  V A,B = Volts  PE A,B = +100J, and q = -1  C What is  V A,B ? AB Higher Potential E Fields point “downhill” with respect to potential difference E field Remember: From A to B!!! +Work

Calculating  V A,B Q is the “source charge.” A is a location near the source charge. r is the distance from the source charge to A.  V A,B =  V ,B -  V ,A A  B Q

Example What is “the potential (V A )” at A, 5cm from a 4 x C point charge? A+4 x C 5cm Q

Example But it is the change in potential that is important. What is the potential difference between point A and point B? B is 10cm from the point charge.  V AB = -360V (the potential at B is less) AB+4 x C 5cm Q

Example A 4g particle with charge q = +6  C is released from rest at A. What is its speed at B? AB  V AB = -360V  PE AB = q  V = (6  C)(-360V ) = -2.2 x J  KE AB = -  PE AB = +2.2 x J =  mv 2 v = 1m/s at location B +4 x C Q

More than one source What is the potential difference  V AB ? All distances are 5cm. AB V A = kq 1 /r 1A + kq 2 /r 2A Sum potentials at A Q 1 = +4 x CQ 2 = +10 x C V A = (9x10 9 )(4x10 -9 )/.05 + (9x10 9 )(10x10 -9 )/.10 V A = 720V + 900V = 1620V V B = (9x10 9 )(4x10 -9 )/.10 + (9x10 9 )(10x10 -9 )/.05 V B = 360V V = 2160V  V AB = +540V potential is higher at B

More than one source AB Q 1 = +4 x CQ 2 = +10 x C  V AB = +540V A 4g particle with charge +6  C is released from rest at B. What is its speed at A?  V BA = -540V  PE BA = q  V = (6  C)(-540V ) = -3.2 x J  KE BA = -  PE BA = +3.2 x J = 1 / 2 mv 2 v = 1.3 m/s at location A q = +6  C

More than one source A Q 1 = +4 x CQ 2 = -4 x C V A = 0 Two contributions add to zero What is the potential at point A midway between these two charges? (different charges than before) Is there an E-field at A? Yes, E net points right. Two contributions add as vectors, yet the potential is zero! E net The potential is negative just right of A and positive just left of A. There is E if V changes.

More than one source A Q 1 = +4 x CQ 2 = -4 x C  V  A = ? How much work do I have to do to bring a 6  C to point A from very far away? The work equals zero also since V  = 0. Depending on the particular path we chose there will be + and - work done along the way but the net work done will always be zero for any path from far away to point A.  V  A = 0