Physics 212 Lecture 5, Slide 1 Physics 212 Lecture 5 Electric Potential Energy.

Slides:



Advertisements
Similar presentations
Electric Potential Mr. Burns
Advertisements

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.
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
Chapter Fourteen The Electric Field and the Electric Potential
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.
Copyright © 2010 Pearson Education, Inc. ConcepTest Clicker Questions Chapter 20 Physics, 4 th Edition James S. Walker.
Physics 2112 Unit 6: Electric Potential
Chapter 22 Electric Potential.
Physics 121: Electricity & Magnetism – Lecture 5 Electric Potential Dale E. Gary Wenda Cao NJIT Physics Department.
PHY 184 Spring 2007 Lecture 10 Title: The Electric Potential, V(x)
Lecture 9 Coulomb’s law Electric field. 3.3 Coulomb’s Law Coulomb’s law gives the force between two point charges: The force is along the line connecting.
General Physics II, Lec 7, By/ T.A. Eleyan 1 Additional Questions ( The Electric Potential )
Norah Ali Al-moneef king saud university
Physics for Scientists and Engineers II, Summer Semester 2009 Lecture 4: May 27 th 2009 Physics for Scientists and Engineers II.
Copyright © 2009 Pearson Education, Inc. Lecture 4 – Electricity & Magnetism b. Electric Potential.
Physics 2102 Lecture 5 Electric Potential I Physics 2102
Lecture 3 Electrical Energy Chapter 16.1  16.5 Outline Potential Difference Electric Potential Equipotential Surface.
Electric Energy and Capacitance
Fall 2008Lecture 1-1Physics 231 Electric Charges, Forces, and Fields.
Chapter 16 Electric Energy and Capacitance. Question I Three equal positive charges are placed on the x-axis, one at the origin, one at x = 2 m, and the.
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Chapter 25 Electric Potential Electrical Potential and Potential Difference When a test charge is placed in an electric field, it experiences a.
AP Physics III.A Electrostatics Origin of Electricity.
AP Physics III.A Electrostatics Origin of Electricity.
Physics 2112 Unit 5: Electric Potential Energy
Question 1 A.a uniformly charged long rod. B.a uniformly charged ring. C.a uniformly charged disk. D.a point charge. Which one of these statements is true?
Chapter 22: Electric Potential
Electric Potential A PowerPoint Presentation by
Electric Fields and Forces AP Physics B. Electric Charge “Charge” is a property of subatomic particles. Facts about charge:
General Physics II, Lec 3, By/ T.A. Eleyan 1 Lecture 3 The Electric Field.
The Electric Potential
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Electric Potential II Physics 2102 Jonathan Dowling Physics 2102 Lecture: 09 MON 02 FEB Ch
Halliday/Resnick/Walker Fundamentals of Physics
Chapter 23 Electric Potential.
Q20. Electric Charge Force and Field
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
MIDTERM 1 UTC Thu-Sep 27, 7:00PM - 9:00PM Course Summary Unit 1 Provided Bring pencils, calculators (memory cleared)
Electric Fields and Forces
AP Physics III.A Electrostatics Origin of Electricity Just two types of charge Magnitude of charge of an electron is the same as that of a proton.
Electric Potential Energy Recall, for point masses, the force of gravity and gravitational potential energy are: and For point charges, it would follow.
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.
 From our studies of work and energy (Chaps. 7 & 8), we know that when a force acts on an object and displaces it, work is done on the object  This also.
Lecture 5 Dr. Lobna Mohamed Abou El-Magd The Electric Potential.
Phys 102 – Lecture 4 Electric potential energy & work.
PHY132 Introduction to Physics II Class 11 – Outline:
Electric Potential.
Chapter 13 Lecture.
Electric Potential Electric Potential Energy Work done by Coulomb force when q 1 moves from a to b: b a FEFE r dr ds q 2 (-) q 1 (+) rara rbrb.
Today’s agenda: Electric potential energy. You must be able to use electric potential energy in work-energy calculations. Electric potential. You must.
Physics 212 Lecture 5, Slide 1 Physics 212 Lecture 5 Today's Concept: Electric Potential Energy Defined as Minus Work Done by Electric Field.
Chapter 25 Electric Potential. Electrical Potential Energy The electrostatic force is a conservative force, thus It is possible to define an electrical.
Potential Difference & Potential Energy MC Fun Problems
Electric Potential 2 q A C B r A B r path independence a a Rr VQ 4   r Q 4   R.
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.
Oct. 4, From last time(s)… Work, energy, and (electric) potential Electric potential and charge Electric potential and electric field. Electric charges,
Chapter 17 Electric Potential. Question 1 answer.
Chapter 25 Electric Potential. Like gravity, the electric force is conservative: it has a Potential Energy. A charge in an electric field has electric.
Key Ideas in Chapter 14: Electric Field  A charged particle makes an electric field at every location in space (except its own location).  The electric.
Electric potential energy. Electric potential.
Electric potential energy. Electric potential.
Question 3. A solid conducting sphere is concentric with a thin conducting shell, as shown. The inner sphere carries a charge Q1, and the spherical shell.
Phys 102 – Lecture 4 Electric potential energy & work.
Phys102 Lecture 6 Electric Potential
Electric Potential Energy
Chapter 23 Electric Potential.
Presentation transcript:

Physics 212 Lecture 5, Slide 1 Physics 212 Lecture 5 Electric Potential Energy

Physics 212 Lecture 5, Slide 2 Recall from physics 211: Fdr W = 0 Constant speed (  K = 0 ) Fdr W > 0 Object speeds up (  K > 0 ) W < 0 Object slows down (  K < 0 ) F drFdr or 9

Physics 212 Lecture 5, Slide 3 Potential Energy If gravity does negative work, potential energy increases! Same idea for Coulomb force… if Coulomb force does negative work, potential energy increases. ++F ++ xxxx Coulomb force does negative work Potential energy increases

Analogy to gravity Work by me = F ext h = - F g h = mgh =  U Exert force F ext = - F g over distance h. Work by me - (Work by gravity) Change in Potential energy h FgFg F ext m m

Physics 212 Lecture 5, Slide 5 Checkpoint 4 A charge is released from rest in a region of electric field. The charge will start to move A) in a direction that makes its potential energy increase B) in a direction that makes its potential energy decrease C) along a path of constant potential energy 34F xxxx It will move in the same direction as F Work done by E field is positive  U = -Work is negative

Physics 212 Lecture 5, Slide 6 FEFEFEFE FHFHFHFHE dr W H is the work done by the hand on the ball W E is the work done by the electric field on the ball Which of the following statements is true: A) W H > 0 and W E > 0 B) W H > 0 and W E 0 and W E < 0 C) W H < 0 and W E < 0 D) W H 0 14 You hold a positively charged ball and walk due west in a region that contains an electric field directed due east. Example: Charge in External Field

Physics 212 Lecture 5, Slide 7 FEFEFEFE FHFHFHFH E dr B) W H > 0 and W E 0 and W E < 0 Conservative force:  U = - W E Not a conservative force. Does not have any  U. Is  U positive or negative? A)Positive B)Negative 16

Move charge q 2 from r 1  r 2. Find the change in potential energy. From the diagram, so, q1q1q1q1 q2q2q2q2 q1q1q1q1 q2q2q2q2

Physics 212 Lecture 5, Slide 9 q1q1q1q1 q2q2q2q2d Calculate the change in potential energy for two point charges originally very far apart, moved to a separation of d. Charged particles w/ same sign have an increase in potential energy when brought closer together. For point charges we often choose r =  as “zero” potential energy. So the potential energy of this configuration is, 19

Physics 212 Lecture 5, Slide 10 Example: Getting the signs right In case A two negative charges which are equal in magnitude are separated by a distance d. In case B the same charges are separated by a distance 2d. Which configuration has the highest potential energy? A) Case A B) Case B d 2d Case A Case B 22

Physics 212 Lecture 5, Slide 11 Example: Getting the signs right As usual, choose U = 0 to be at infinity:As usual, choose U = 0 to be at infinity: U(r) 0 r d Case A U(d) 2d Case B U(2d) U A > U B 23

Physics 212 Lecture 5, Slide 12 Checkpoint 1 34 A B C D E Note: +q moves AWAY from +Q. Its potential energy MUST DECREASE  U < 0

Physics 212 Lecture 5, Slide 13 Potential Energy of Many Charges Two charges are separated by a distance d. What is the change in potential energy when a third charge q is brought from far away to a distance d from the original two charges? Q1Q1Q1Q1 Q2Q2Q2Q2 25 (superposition) d q d d

Physics 212 Lecture 5, Slide 14 Potential Energy of Many ChargesQQ d Q 27 dd Work (by me) to bring in second charge : Work (by me) to bring in first charge: W 1 = 0 Work (by me) to bring in third charge : What is the total energy required to bring in three identical charges, from infinitely far away to the points on an equilateral triangle shown ?

Physics 212 Lecture 5, Slide 15 Potential Energy of Many Charges Suppose one of the charges is negative. Now what is the total energy required to bring the three charges in infinitely far away? A) 0 B) C) D) E) QQ d -Q 29 dd Work to bring in third charge : Work to bring in first charge: W 1 = 0 1 Work to bring in second charge : 3 2

Physics 212 Lecture 5, Slide 16 Checkpoint 2 31 A B C D A B C D

Physics 212 Lecture 5, Slide 17 Checkpoint 3 34 LET’S DO THE CALCULATION !!

Physics 212 Lecture 5, Slide 18 Example: Potential Energy Changes A positive charge q is placed at x=0 and a negative charge -2q is placed at x=d. At how many different places along the x axis could another positive charge be placed without changing the total potential energy of the system? 37 q -2q x X=0 X=d A)0 B)1 C)2 D)3

Physics 212 Lecture 5, Slide 19 Example: Potential Energy Changes At which two places can a positive charge be placed without changing the total potential energy of the system? 40 q -2q A BC D x X=0 X=d A)A & B B)A & C C)B & C D)B & D E)A & D Let’s calculate the positions of A and B

Physics 212 Lecture 5, Slide 20 Lets work out where A is 43 q -2q A x X=0 X=d d r Set  U = 0 Makes Sense! Q is twice as far from -2q as it is from +q

Physics 212 Lecture 5, Slide 21 Lets work out where B is 46 q -2q B x X=0 X=d d - r r Setting  U = 0 Makes Sense! Q is twice as far from -2q as it is from +q

Physics 212 Lecture 5, Slide 22 Summary q1q1 q2q2 r For a pair of charges: For a collection of charges: Sum up for all pairs Just evaluate (We usually choose U = 0 to be where the charges are far apart)