Electricity and Magnetism

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

Work and Energy Partial Derivatives. Work The force can be three dimensional.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 24.
Hw: All Chapter 3 problems and exercises Reading: Chapter 4.
Work done by electric force (source: fixed charges) on a test charge depends only on endpoints, not on path. (You can see this easily for a single fixed.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 18.
Ch3 Quiz 1 First name ______________________ Last name ___________________ Section number ______ There is an electric field given by where E 0 is a constant.
A charged particle with positive charge q 1 is fixed at the point x=a, y=b. What are the x and y components of the force on a particle with positive charge.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 21.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 14.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 24.
Hw: All Chapter 3 problems and exercises Reading: Chapter 3.
Chapter 2 hw quiz What is the electric field at the center of a circle of radius R if the top half of the circle has a uniform charge +Q spread over the.
Chapter 7 All forces are CONSERVATIVE or NON-CONSERVATIVE.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 10.
Instructor: Dr. Tatiana Erukhimova
Nobel Prize in Physics 2008 Yoichiro Nambu Makoto Kobayashi Toshihide Maskawa "for the discovery of the mechanism of spontaneous broken symmetry in subatomic.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Sections 801, 802, 803 Lecture 3.
LCROSS crashes into the Moon. Image credit: NASA.
Chapter 3. Electric Potential Constant electric field The Electric Potential: V - Single Charge - Dipole - conservative? potential energy function?
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 22.
22-1 Physics I Class 22 Electric Potential Work Integral in Multiple Dimensions (Review)
Example 6: Electric field on disk’s axis z Example 2 Consider a constant, vertical electric field somehow created in a limited region of space. An electron.
2D case: If or then 2 or 3D cases: Several dimensions: U(x,y,z) Compact notation using vector del, or nabla: Another notation: Partial derivative is.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 20.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 27.
A charged particle with positive charge q 1 is fixed at the point x=a, y=b. What are the x and y components of the force on a particle with positive charge.
Hw: All Chapter 4 problems and exercises Chapter 5: Pr. 1-4; Ex. 1,2 Reading: Chapter 4.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 23.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 26.
Day18: Electric Dipole Potential & Determining E-Field from V
A charged particle with positive charge q 1 is fixed at the point x=a, y=b. y x q1q1 q2q2 a c d b What are the x and y components of the force on a particle.
2D case: If or then 2 or 3D cases: Several dimensions: U(x,y,z) Compact notation using vector del, or nabla: Another notation: Partial derivative is.
Lecture 5 Dr. Lobna Mohamed Abou El-Magd The Electric Potential.
Chapter 18 Section 18.4 Another Notation for Line Integrals.
Chapter 21 Electric Potential.
A charged particle with positive charge q 1 is fixed at the point x=a, y=b. What are the x and y components of the force on a particle with positive charge.
Multiplication of vectors Two different interactions (what’s the difference?)  Scalar or dot product : the calculation giving the work done by a force.
Chapter 17 Electric Potential. Question 1 answer.
Problem 3 p. 45 Electric potential on ring’s axis From Chapter 2:
Electricity and Magnetism
Electric Fields and Potential
Electricity and Magnetism
Instructor: Dr. Tatiana Erukhimova
ENE/EIE 325 Electromagnetic Fields and Waves
Instructor: Dr. Tatiana Erukhimova
Electricity and Magnetism
Electric Fields and Potential
Electricity and Magnetism
PHYS 241 Recitation Kevin Ralphs Week 4.
Electricity and Magnetism
Electricity and Magnetism
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Electricity and Magnetism
Instructor: Dr. Tatiana Erukhimova
PHYS 241 Recitation Quiz Kevin Ralphs Week 2.
Electricity and Magnetism
Electricity and Magnetism
Instructor: Dr. Tatiana Erukhimova
Electricity and Magnetism
Electricity and Magnetism
Instructor: Dr. Tatiana Erukhimova
Electricity and Magnetism
Electricity and Magnetism
Electricity and Magnetism
Electricity and Magnetism
Electricity and Magnetism
Electricity and Magnetism
Instructor: Dr. Tatiana Erukhimova
Presentation transcript:

Electricity and Magnetism Physics 208 Dr. Tatiana Erukhimova Lecture 8

P218 Review: Conservative forces One-dimensional problem:

Two-dimensional problem: does NOT depend on path! around the closed path is zero!

Chapter 3. Electric Potential Constant electric field The Electric Potential: V - Single Charge - Dipole - conservative? potential energy function?

For a point charge at the origin:

There is an electric field given by Ch3 Quiz 1 There is an electric field given by where E0 is a constant. What is the difference in the value of the electric potential due to this electric field between the origin and the point x=a, y=b?

There is an electric field given by Ch3 Quiz 2 There is an electric field given by where  and  are constants. What is the difference in the value of the electric potential due to this electric field between the origin and the point x=a, y=b?

where c is a constant and r is the distance from the origin; Ch3 Quiz 3 There is an electric field created by some source at the origin given by where c is a constant and r is the distance from the origin; points out from the origin. What is the difference in the value of the electric potential due to this electric field between the point x=a, y=b and the point at infinity? What is the potential function corresponding to this electric field if instead of being at the origin the source of the electric field is at point x=a, y=b?

2D case:

2 or 3D cases: If or then

Several dimensions: U(x,y,z) Partial derivative is taken assuming all other arguments fixed Compact notation using vector del, or nabla: Another notation:

Geometric meaning of the gradient Direction of the steepest ascent; Magnitude : the slope in that direction Direction of the steepest descent Magnitude : the slope in that direction http://reynolds.asu.edu/topo_gallery/topo_gallery.htm

Have a great day! Hw: All Chapter 3 problems and exercises Reading: Chapter 4