Phys 133 Chapter 26 Electric Field. Phys 133 Electric Field A creates field in space changes the environment B interacts with field New long range interaction.

Slides:



Advertisements
Similar presentations
Chapter 22: The Electric Field II: Continuous Charge Distributions
Advertisements

Continuous Charge Distributions
Electric Charges and Electric Fields
Chapter 28 Electric Potential Phys 133 – Chapter 30.
Chapter 28. Magnetic Field
Chapter 30 Sources of the magnetic field
Chapter 27 Sources of the magnetic field
PHY132 Introduction to Physics II Class 10 – Outline:
CHAPTER 23 : ELECTRIC FIELDS
Chapter 23 Gauss’ Law.
Chapter 22 Electric Potential.
Chapter 23 Summer 1996, Near the University of Arizona Chapter 23 Electric Fields.
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Question A) B) C) D) E An electric field polarizes a metal block as shown.
Chapter 26.
ELECTRICITY PHY1013S ELECTRIC FIELDS Gregor Leigh
Chapter 24 Capacitance, Dielectrics, Electric Energy Storage
UNIVERSITI MALAYSIA PERLIS
Chapter 22: Electric Fields
Chapter 22 Electric Field
Chapter 25 Electric Potential Electrical Potential and Potential Difference When a test charge is placed in an electric field, it experiences a.
Electric Charge and Electric Field
Chapter 21 Gauss’s Law. Electric Field Lines Electric field lines (convenient for visualizing electric field patterns) – lines pointing in the direction.
1 Electric Field – Continuous Charge Distribution As the average separation between source charges is smaller than the distance between the charges and.
Electric Flux and Gauss Law
R 2R2R a a Today… More on Electric Field: –Continuous Charge Distributions Electric Flux: –Definition –How to think about flux.
Physics 1202: Lecture 3 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
Chapter 22 Gauss’s Law Chapter 22 opener. Gauss’s law is an elegant relation between electric charge and electric field. It is more general than Coulomb’s.
Electric Field Models The electric field of a point charge q at the origin, r = 0, is where є 0 = 8.85 × 10 –12 C 2 /N m 2 is the permittivity constant.
23.1 THE ELECTRIC FIELD The electric field strength E: E=F/q t (23.1) Any charged particle does not interact directly with other charged particle; rather,
General Physics II, Lec 3, By/ T.A. Eleyan 1 Lecture 3 The Electric Field.
Electric Potential Chapter 25. ELECTRIC POTENTIAL DIFFERENCE The fundamental definition of the electric potential V is given in terms of the electric.
Physics 2113 Lecture 08: MON 02 FEB Electric Fields III Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb ( )
CHAPTER OUTLINE 30.1 The Biot–Savart Law 30.2 The Magnetic Force Between Two Parallel Conductors 30.3 Ampère’s Law 30.4 The Magnetic Field of a Solenoid.
Halliday/Resnick/Walker Fundamentals of Physics
Day 4: Electric Field Calculations for Continuous Charge Distributions A Uniform Distribution of Surface charge A Ring of Continuous Charge A Long Line.
Chapter 21 Electric Charge and Electric Field
Question. Question A) B) C) D) E An electric field polarizes a metal.
Wednesday, Sep. 14, PHYS Dr. Andrew Brandt PHYS 1444 – Section 04 Lecture #5 Chapter 21: E-field examples Chapter 22: Gauss’ Law Examples.
-Electric Potential due to Continuous Charge Distributions AP Physics C Mrs. Coyle.
Electric Field.
Electric Field formulas for several continuous distribution of charge.
Lecture 19 Electric Potential
Electric Potential.
Conductor, insulator and ground. Force between two point charges:
Copyright © 2009 Pearson Education, Inc. Supplemental Lecture Taken from Ch. 21 in the book by Giancoli Section & Example Numbers refer to that book.
Review on Coulomb’s Law and the electric field definition Coulomb’s Law: the force between two point charges The electric field is defined as The force.
Thursday, Sept. 8, 2011PHYS , Fall 2011 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #6 Thursday, Sept. 8, 2011 Dr. Jaehoon Yu Chapter 21 –Electric.
Chapter 22 Electric Fields The Electric Field: The Electric Field is a vector field. The electric field, E, consists of a distribution of vectors,
Copyright © 2009 Pearson Education, Inc. Biot-Savart Law.
Review on Coulomb’s Law and the electric field definition
Chapter 25 Electric Potential.
Announcements – 272H EXAM 1 – Thursday, Feb. 13, 8-9:30 pm in room 203 –Chapters 14, 15, & 16 –Equation sheet will be provided –Pencil, calculator There.
Electric Fields Due to Continuous Charge Distributions
Unimportable clickers:
Chapter 23: Electric Fields
Last Time Insulators: Electrons stay close to their own atoms
Electric Fields AP Physics C.
Physics 122B Electricity and Magnetism
Electric Fields AP Physics C.
ELECTRIC FIELD ELECTRIC FLUX Lectures 3, 4 & 5 a a R 2R
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Lecture 10 Biot-Savart’s Law.
Physics 2113 Lecture 07: WED 09 SEP
Chapter 22 Electric Field
Electric Field Models The electric field of a point charge q at the origin, r = 0, is where є0 = 8.85 × 10–12 C2/N m2 is the permittivity constant. The.
Electric field of distributed charges
Chapter 16 Electric Field of Distributed Charges
Chapter 23 Electric Field Phys 133.
Physics 122B Electricity and Magnetism
Presentation transcript:

Phys 133 Chapter 26 Electric Field

Phys 133 Electric Field A creates field in space changes the environment B interacts with field New long range interaction

Phys 133 Place test charge Find force remove test charge Procedure

Phys 133 Simulation: Electric Field

Phys 133 Understanding Fields (in general) Vector field worksheet (field at tail, relative lengths)

Phys 133 Vector field worksheet (cont.)

Phys 133 Vector field worksheet (ans)

Phys 133 Positive point chargeNegative point charge Radial from source, depends on distance Electric Field: point charge

Phys 133 Electric Field (multiple charges) Net force at some point is sum of the forces due to all objects around Defined or Therefore,

Phys 133 Do workbook 26.5ac, 7adf

Phys 133 Electric field of a dipole along the y-axis…

Phys 133 Electric field of a dipole along the y-axis…

Phys 133 Electric field of a dipole along the y-axis What is the electric field of a dipole for y >> d?

Phys 133 Vector Field and Field Lines Two ways to describe the same thing Dipole with +/- Vector fieldField lines

Phys 133 Dipole with +/+ Vector field Field lines More Vector Field and Field Lines

Phys 133 Electric Field lines Rank the electric field strength in order from largest to smallest. A: E 1 < E 2 < E 3 = E 4 B: E 3 = E 4 < E 2 < E 1 C: E 2 = E 3 < E 4 < E 1 D: E 1 < E 4 < E 2 = E 3

Phys 133 Electric Field of a “blob”

Phys 133 Charge Density Charge Q is spread uniformly on a rectangle of sides a and b. a) What is the surface charge density? b) The original rectangle, #1, is then broken into two smaller rectangles, #2 and #3. Compare the surface charge densities,  1,  2,  3. and the charges Q 1, Q 2, Q 3.

Phys 133 Charge Density ans Charge Q is spread uniformly on a rectangle of sides a and b. a) What is the surface charge density? b) The original rectangle, #1, is then broken into two smaller rectangles, #2 and #3. Compare the surface charge densities,  1,  2,  3. Charge is uniformly spread over rectangle. Piece #2 has a 1/3 the area, so 1/3 the charge.

Phys 133 Electric Field (continuous distribution) P (i) th bit of charge

Phys 133  Draw a picture, pick a coordinate system.  Identify, P, the place in space you want the field.  Pick a generic (no special points) chunk of charge  Q for which you know the field.  Determine the components of (E x, E y, …) at P due to chunk expressed in terms of variables (x, y, …r,  …).  Express the charge  Q in terms of charge density and infinitesimal variable(s) (dz, d  …)  Express all quantities (angles, distances, etc.) in terms of coordinates.  Add up contributions, sum becomes definite integral with limits corresponding to charge.  Evaluate integral and simplify result as much as possible. Strategy

Phys 133 A thin rod of length L and charge Q. Find components of the electric field vector along the dotted line. Problem

Phys 133 Problem ans x y Draw a picture, pick a coordinate system.Identify, P, the place in space you want the field. Pick a generic chunk of charge  Q. i th Determine the components of (E x, E y, …) at P due to chunk expressed in terms of variables (x, y, …r,  …). P Express the charge  Q in terms of charge density and infinitesimal variable(s) (dz, d  …) Express all quantities (angles, distances, etc.) in terms of coordinates. x

Phys 133 Add up contributions, sum becomes definite integral with limits corresponding to charge. Problem ans x

Phys 133 Add up contributions, sum becomes definite integral with limits corresponding to charge. Problem ans y

Phys 133 Problem ans complete

Phys 133 A plastic rod with linear charge density is bent into a quarter circle. Find the electric field at the origin. a)Write expressions for x and y components of field due to a small piece at angle . b)Write integrals for the components of total field. c)Evaluate, find Problem 26.49

Phys 133 Problem ans (i) th bit of charge

Phys 133 Field of quarter circle of charge

Phys 133 Other charge geometries Line Hoop Disk (from hoops) Plane (from disk)

Phys 133 Points directly away, decrease with distance Field of line (infinite)

Phys 133 Field of hoop, along axis

Phys 133 Field of disk, along axis

Phys 133 perpendicular to the plane Field of plane (“infinite”)

Phys 133 Straighten up, no distance dependence Plane from lots of lines (perpendicular to page)

Phys 133 Parallel-plate Capacitor Net charge is zero Charge lost from +Q side ends up on -Q side

Phys 133 Find the electric field inside capacitor

Phys 133

Charges in an Electric Field Electric Field (due to charges; we can calculate) Charge in Electric Field (experiences a force)

Phys 133 Do Workbook & 31

Phys 133 A proton traveling at a speed of 1.0x10 6 m/s enters the gap between the plates of a 2.0-cm wide parallel plate capacitor. The plates have a surface charge density of +/- 1.0x10 -6 C/m 2. How far is the proton deflected when reaching far end of capacitor? (Ans: 2.2 mm) e=1.6 x C; m p =1.67 x kg;  o =8.85 x C 2 /N-m 2 Problem 26.52

Phys 133 Dipole in an Electric Field

Phys 133