9: Consider an electric dipole where the positive charge, +q, is located on the positive z axis a distance d/2 above the x - y plane, and the negative charge, -q, is located on the negative z axis a distance d/2 below the xy plane, as shown. If the evaluation point is at a distance which is very large as compared to the separation between the charges, then the form of the expression for the net electric field has a very simplified form in terms of the electric dipole moment (EDM). k +91 d/2 -q Ε Part (a) Enter an exact expression for the magnitude of the vector Ẽ, the contribution of the positive charge to the electric field at the point (0, 0, z) where z> d/2. |E|=z (d/2) X Attempts Remain o Part (b) Enter an exact expression for the magnitude of the vector Ẽ, the contribution of the negative charge to the electric field at the point (0, 0, z) where z> d/2. result. Part (c) Enter an exact expression for the total electric field vector Ēnet, at the point (0, 0, 2). Part (d) Notice that when z »d, then z²±d²/4 z². Use this approximation to simplify your expression from the previous part. Enter your vector Part (e) The EDM (electric dipole moment) is represented by a vector, p. The magnitude of the vector is the product of the positive charge and the separation between the charges. The direction is from the negative and towards the positive charge. Rewrite your vector expression for the electric field of the dipole in terms of the EDM, p. Ē net view
9: Consider an electric dipole where the positive charge, +q, is located on the positive z axis a distance d/2 above the x - y plane, and the negative charge, -q, is located on the negative z axis a distance d/2 below the xy plane, as shown. If the evaluation point is at a distance which is very large as compared to the separation between the charges, then the form of the expression for the net electric field has a very simplified form in terms of the electric dipole moment (EDM). k +91 d/2 -q Ε Part (a) Enter an exact expression for the magnitude of the vector Ẽ, the contribution of the positive charge to the electric field at the point (0, 0, z) where z> d/2. |E|=z (d/2) X Attempts Remain o Part (b) Enter an exact expression for the magnitude of the vector Ẽ, the contribution of the negative charge to the electric field at the point (0, 0, z) where z> d/2. result. Part (c) Enter an exact expression for the total electric field vector Ēnet, at the point (0, 0, 2). Part (d) Notice that when z »d, then z²±d²/4 z². Use this approximation to simplify your expression from the previous part. Enter your vector Part (e) The EDM (electric dipole moment) is represented by a vector, p. The magnitude of the vector is the product of the positive charge and the separation between the charges. The direction is from the negative and towards the positive charge. Rewrite your vector expression for the electric field of the dipole in terms of the EDM, p. Ē net view
College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
Related questions
Question
100%
Plz don't use chat gpt
Solve correctly all parts

Transcribed Image Text:9: Consider an electric dipole where the positive charge, +q, is located on the positive z axis
a distance d/2 above the x - y plane, and the negative charge, -q, is located on the negative z axis a distance
d/2 below the xy plane, as shown. If the evaluation point is at a distance which is very large as compared to
the separation between the charges, then the form of the expression for the net electric field has a very
simplified form in terms of the electric dipole moment (EDM).
k
+91
d/2
-q
Ε
Part (a) Enter an exact expression for the magnitude of the vector Ẽ, the contribution of the positive charge to the electric field at the point (0, 0, z)
where z> d/2.
|E|=z (d/2) X Attempts Remain
o Part (b) Enter an exact expression for the magnitude of the vector Ẽ, the contribution of the negative charge to the electric field at the point (0, 0, z)
where z> d/2.
result.
Part (c) Enter an exact expression for the total electric field vector Ēnet, at the point (0, 0, 2).
Part (d) Notice that when z »d, then z²±d²/4 z². Use this approximation to simplify your expression from the previous part. Enter your vector
Part (e) The EDM (electric dipole moment) is represented by a vector, p. The magnitude of the vector is the product of the positive charge and the
separation between the charges. The direction is from the negative and towards the positive charge. Rewrite your vector expression for the electric field of the dipole
in terms of the EDM, p.
Ē
net
view
Expert Solution

This question has been solved!
Explore an expertly crafted, step-by-step solution for a thorough understanding of key concepts.
This is a popular solution!
Trending now
This is a popular solution!
Step by step
Solved in 2 steps with 3 images

Recommended textbooks for you

College Physics
Physics
ISBN:
9781305952300
Author:
Raymond A. Serway, Chris Vuille
Publisher:
Cengage Learning

University Physics (14th Edition)
Physics
ISBN:
9780133969290
Author:
Hugh D. Young, Roger A. Freedman
Publisher:
PEARSON

Introduction To Quantum Mechanics
Physics
ISBN:
9781107189638
Author:
Griffiths, David J., Schroeter, Darrell F.
Publisher:
Cambridge University Press

College Physics
Physics
ISBN:
9781305952300
Author:
Raymond A. Serway, Chris Vuille
Publisher:
Cengage Learning

University Physics (14th Edition)
Physics
ISBN:
9780133969290
Author:
Hugh D. Young, Roger A. Freedman
Publisher:
PEARSON

Introduction To Quantum Mechanics
Physics
ISBN:
9781107189638
Author:
Griffiths, David J., Schroeter, Darrell F.
Publisher:
Cambridge University Press

Physics for Scientists and Engineers
Physics
ISBN:
9781337553278
Author:
Raymond A. Serway, John W. Jewett
Publisher:
Cengage Learning

Lecture- Tutorials for Introductory Astronomy
Physics
ISBN:
9780321820464
Author:
Edward E. Prather, Tim P. Slater, Jeff P. Adams, Gina Brissenden
Publisher:
Addison-Wesley

College Physics: A Strategic Approach (4th Editio…
Physics
ISBN:
9780134609034
Author:
Randall D. Knight (Professor Emeritus), Brian Jones, Stuart Field
Publisher:
PEARSON