Electric Field & Electric Potential

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Video Clips

Video RealVideo®
5:16 minutes (0:00 - 5:16)

Definition, with examples of electric field around a positive charge and a negative charge.

Prior Knowledge: Electric Force, Coulomb's Law (29:30 of video lecture 1)
Instructor: Prof. Walter Lewin
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Video RealVideo®
6:29 minutes (5:16 - 11:45)

Finding the electric field due to more than one charge using the superposition principle, with the example of the electric field of a positive charge next to a negative charge.

Prior Knowledge: Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Instructor: Prof. Walter Lewin
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Video RealVideo®
6:13 minutes (11:45 - 17:58)

Graphical representation of the electric field for an arrangement of a +3 charge next to a -1 charge, first using arrows and then using electric field lines. Definition and discussion of electric field lines.

Prior Knowledge: Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Instructor: Prof. Walter Lewin
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Video RealVideo®
2:41 minutes (17:58 - 20:39)

Comparison between force due to gravity on earth and force on a charge in a uniform electric field. Electric field lines indicate direction of force on a charge, they are not trajectories.

Prior Knowledge: Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Instructor: Prof. Walter Lewin
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Video RealVideo®
1:49 minutes (20:39 - 22:28)

The electric field for two charges with the same polarity, using the example of like charges with magnitudes 4 and 1.

Prior Knowledge: Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Instructor: Prof. Walter Lewin
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Video RealVideo®
4:05 minutes (22:28 - 26:33)

Definition, including a representation of the electric field for a dipole. Atoms or molecules can become induced dipoles when placed in an electric field.

Prior Knowledge: Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Instructor: Prof. Walter Lewin
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Video RealVideo®
6:36 minutes (26:33 - 33:09)

Using a charged rubber rod and two metal spheres to create a dipole. An electroscope is used to show that a dipole has been created.

Prior Knowledge: Dipoles (22:28 of video lecture 2), Electroscopes (42:00 of video lecture 1)
Instructor: Prof. Walter Lewin
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Video RealVideo®
7:47 minutes (33:09 - 40:56)

Torque on a dipole in an electric field causes it to rotate and align with the field. Demonstration by creating a dipole and placing it in the electric field of a large Van de Graaff generator.

Prior Knowledge: Dipoles (22:28 of video lecture 2), Electric Field (beginning of video lecture 2)
Instructor: Prof. Walter Lewin
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Video RealVideo®
4:48 minutes (40:56 - 45:44)

Demonstration of using grass seeds in oil to probe an electric field, with examples of the field for a dipole and for two charges of the same polarity.

Prior Knowledge: Electric Field (beginning of video lecture 2)
Instructor: Prof. Walter Lewin
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Video RealVideo®
3:40 minutes (45:44 - 49:24)

Using a balloon to demonstrate the electric field between a Van de Graaff generator and an oppositely charged Professor Walter Lewin.

Prior Knowledge: Electric Field (beginning of video lecture 2)
Instructor: Prof. Walter Lewin
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Video RealVideo®
7:11 minutes (0:00 - 7:11)

Calculating the electric flux through a surface by breaking it into small areas dA and integrating over the surface. Comparison between electric flux and air flow, with a diagram. Definition of a closed surface.

Prior Knowledge: Electric Field (beginning of video lecture 2)
Instructor: Prof. Walter Lewin
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Video RealVideo®
7:14 minutes (0:00 - 7:14)

Definition, work required to bring charges from infinity into a specific arrangement. Conservative forces, just like gravity.

Prior Knowledge: Electric Field (beginning of video lecture 2)
Instructor: Prof. Walter Lewin
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Video RealVideo®
3:49 minutes (7:14 - 11:03)

Definition, work per unit charge to move from infinity to a specific location. Measured in volts.

Prior Knowledge: Electric Field (beginning of video lecture 2) and Electrostatic Potential Energy (beginning of video lecture 4)
Instructor: Prof. Walter Lewin
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Video RealVideo®
8:31 minutes (18:12 - 26:43)

Finding the potential around an arrangement of multiple point charges, with examples of a pair of positive charges and a pair of charges with opposite polarity. Field lines are always parallel to equipotential surfaces, and equipotential surfaces with different potentials can never intersect.

Prior Knowledge: Electric Potential (7:14 of video lecture 4)
Instructor: Prof. Walter Lewin
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Video RealVideo®
2:44 minutes (26:43 - 29:27)

Sometimes it is easier to work with potential difference rather than a complicated electric field. Distinction between potential V and potential energy U; do not confuse the two. Positive charges move from high to low potential energy, negative charges do the opposite.

Prior Knowledge: Electric Potential (7:14 of video lecture 4)
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Video RealVideo®
12:03 minutes (29:27 - 41:30)

Finding the difference in electric potential between two points A and B. Finding the change in kinetic energy from the potential difference. Any piece of metal is an equipotential surface, with example of a metal trash can attached to point A and a soda can attached to point B.

Prior Knowledge: Electric Potential (7:14 of video lecture 4)
Instructor: Prof. Walter Lewin
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Video RealVideo®
1:27 minutes (41:30 - 42:57)

Potentials are generally defined relative to infinity, but often it doesn't matter where potential is defined to be zero because only the change in potential has any real meaning.

Prior Knowledge: Electric Potential (7:14 of video lecture 4)
Instructor: Prof. Walter Lewin
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Video RealVideo®
6:04 minutes (42:57 - 49:01)

Using a large Van de Graaff generator and a fluorescent tube to show that there is a very large potential difference in a strong electric field.

Prior Knowledge: Electric Potential (7:14 of video lecture 4)
Instructor: Prof. Walter Lewin
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Video RealVideo®
6:00 minutes (0:00 - 6:00)

Relationship between electric field and electric potential.

Prior Knowledge: Electric Field (beginning of video lecture 2) and Electric Potential (7:14 of video lecture 4)
Instructor: Prof. Walter Lewin
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Video RealVideo®
3:37 minutes (6:00 - 9:37)

Field lines are perpendicular to equipotential surfaces. It takes no work to move charge perpendicular to the electric field. Comparison to contour lines on a ski mountain.

Prior Knowledge: Electric Field (beginning of video lecture 2) and Electric Potential (7:14 of video lecture 4)
Instructor: Prof. Walter Lewin
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Video RealVideo®
4:08 minutes (9:37 - 13:45)

Finding potential from the components of the electric field. Gradient is defined.

Prior Knowledge: Electric Field (beginning of video lecture 2) and Electric Potential (7:14 of video lecture 4)
Instructor: Prof. Walter Lewin
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Video RealVideo®
6:48 minutes (13:45 - 20:33)

Finding the electric field when potential is (10^5)*x in the x direction.

Prior Knowledge: Electric Field (beginning of video lecture 2) and Electric Potential (7:14 of video lecture 4)
Instructor: Prof. Walter Lewin
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Video RealVideo®
5:08 minutes (44:27 - 49:35)

Finding the increase in kinetic energy when an electron is moved across a potential difference.

Prior Knowledge: Kinetic Energy (from 8.01)
Instructor: Prof. Walter Lewin
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How Your Heart Works Pt. 1 (8.02 Spring 2002)

Video RealVideo®
8:53 minutes (3:00 - 11:53)

How changing potentials in heart cells keep the heart pumping.

Prior Knowledge: None
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Video RealVideo®
8:37 minutes (11:53 - 20:30)

Electrocardiograms, defibrillators, and pacemakers are explained, including a demonstration of an electrocardiogram on a student.

Prior Knowledge: How Your Heart Works Pt. 1 (3:00 of video lecture 19)
Instructor: Prof. Walter Lewin
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Lecture Notes

Document PDF
Page 51 to page 54

Definition, with link to a visualization.

Prior Knowledge: Fields and Coulomb's Law (pages 26-50 from presentation 1)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 1 to page 7

Comparison of gravitational and electric fields. Electric field lines defined with diagrams. Example problem without solution.

Prior Knowledge: Electric Charge and Field (pages 45-54 from presentation 1)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 17 to page 28

Potential and potential energy for electrostatics compared to same concepts for gravity. Volt is defined as the unit for potential difference. Potential landscapes illustrated by diagram. Equation for potential created by a point charge.

Prior Knowledge: Gravitational Potential and Potential Energy (pages 10-16 of presentation 4)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 29 to page 32

Derivation of electric field as the gradient of potential

Prior Knowledge: Electric Potential (pages 17-28 of presentation 4) and Electric Field (pages 45-54 of presentation 1)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 33 to page 36

Energy required to bring charges from infinity into a specific arrangement. Examples for 2 and 3 point charges.

Prior Knowledge: Electric Potential (pages 17-28 of presentation 4)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 1 to page 6

Relationship between electric field and electric potential for point charges.

Prior Knowledge: Electric Potential (pages 17-36 of presentation 4)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 42 to page 47

Finding electric potential using electric fields calculated from Gauss's Law. Worked example with diagrams of a nonconducting sphere of uniform charge.

Prior Knowledge: Electric Fields, Potential, and Gauss's Law (pages 1-41 of presentation 5)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF#
Page 14 to page 18

Electric potential; Lorentz force and magnetic force; Biot-Savart Law; magnetic dipole moments

Prior Knowledge: Material is from presentations 1-5 and 14-20.
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF#
Page 27 to page 32

Finding the electric field, electric potential, magnetic field, and field energy between the plates of a charging capacitor.

Prior Knowledge: Gauss's Law (pages 7-22 of presentation 5) and Ampere's Law (pages 21-26 of presentation 18)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 1 to page 3

Scalar fields and vector fields are defined, with diagrams and examples. Brief review of gravitational field and introduction to electric field, with important equations for each.

Prior Knowledge: None
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 1 to page 2

Definitions, with equations. Superposition, charge densities, and unit vectors are also defined.

Prior Knowledge: Fields (R1)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 1 to page 2

Definitions, with equations and properties.

Prior Knowledge: Electric Charge and Field (R2)
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 4 to page 7

Definition; field lines; fields for ring and disk of charge.

Prior Knowledge: Coulomb's Law
Instructor: Prof. Gabriella Sciolla
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Online Textbook Chapters

Document PDF
Page 16 to page 19

Showing fields through arrows, field lines, grass seeds, and iron filings; motion of fields.

Prior Knowledge: Vector fields
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 7 to page 11

Definition; fields for point charges and field lines; force from fields.

Prior Knowledge: Coulomb's Law
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 2 to page 6

Definition; gravitational work and conservative forces; potential and potential energy for gravity.

Prior Knowledge: Electric fields
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 6 to page 10

Defined for E-fields and calculated for point charges and continuous distributions.

Prior Knowledge: Work and potential
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Page 10 to page 13

Deriving E-field from potential; equipotential surfaces defined.

Prior Knowledge: Electric potential
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Practice Problems

Document PDF
Problem 16 to problem 17

Question about the electric field for two unequal point charges with opposite signs, with answer and explanation.

Prior Knowledge: None
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Problem 1 to problem 4

Two questions with answers and explanations.

Prior Knowledge: None
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Problem 5 to problem 8

Two questions with answers and explanations.

Prior Knowledge: None
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Problem 9 to problem 12

Question about electric field of a dipole, with answer and explanation. Question about force on a dipole in an electric field, with answer and explanation.

Prior Knowledge: None
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Problem 1 to problem 2

Question with answer and explanation.

Prior Knowledge: None
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Problem 3 to problem 12

Five questions with answers and explanations.

Prior Knowledge: None
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Problem 7 to problem 10

Two questions about determining the electric field when the electric potential is known, with answers and explanations.

Prior Knowledge: None
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Problem 1 to problem 2

Question about walking down a mountain most quickly, with answer and explanation.

Prior Knowledge: None
Instructors: Prof. John Belcher, Dr. Peter Dourmashkin, Prof. Michael Feld, Prof. Eric Hudson, Prof. John Joannopoulos, Prof. Bruce Knuteson, Dr. George Stephans
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Document PDF
Problem 2

3-part E-field problem; calculating and plotting E-field along x-axis.

Prior Knowledge: None
Instructor: Prof. Walter Lewin
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Document PDF
Problem 2

3-part Gauss's law problem; finding radial E-field and potential.

Prior Knowledge: None
Instructor: Prof. Walter Lewin
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Problem 4

6-part point charge problem; e-fields and potentials from point charge distribution; potential and kinetic energy.

Prior Knowledge: None
Instructor: Prof. Walter Lewin
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Document PDF
Problem 6

4-part voltage problem; finding radius and voltage of charged sphere.

Prior Knowledge: None
Instructor: Prof. Walter Lewin
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Document PDF#
Problem 3

Finding position for third charge to cancel second; reaction to perturbation.

Prior Knowledge: None
Instructors: Dr. Peter Dourmashkin, Prof. Gunther Roland
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Document PDF
Problem 3

Finding F and τ on dipole from E-field; charge of point from motion of dipole; acceleration from point charge force.

Prior Knowledge: None
Instructors: Dr. Peter Dourmashkin, Prof. Gunther Roland
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Document PDF
Problem 1

Comparing potential and potential energy of opposite charges near a fixed point charge.

Prior Knowledge: None
Instructors: Dr. Peter Dourmashkin, Prof. Gunther Roland
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Problem 2

Calculating initial speed of proton given distance traveled to nucleus.

Prior Knowledge: None
Instructors: Dr. Peter Dourmashkin, Prof. Gunther Roland
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Problem 3

Explaining equipotentiality; comparing E-fields near spheres.

Prior Knowledge: None
Instructors: Dr. Peter Dourmashkin, Prof. Gunther Roland
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Problem 1

4-part problem; finding force on one charge, E-field along x-axis and y-axis, graphing, and drawing field lines.

Prior Knowledge: None
Instructors: Dr. Peter Dourmashkin, Prof. Gunther Roland
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Problem 2

Graphing and approximating electric potential; graphing potential energy.

Prior Knowledge: None
Instructors: Dr. Peter Dourmashkin, Prof. Gunther Roland
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Exam Questions

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Problem 3

Finding field lines for E-field with given effect on dipole; F and τ on dipole for greater negative charge.

Prior Knowledge: None
Instructors: Dr. Peter Dourmashkin, Prof. Gunther Roland
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Problem 1

For triangular arrangement of charges, finding the E-field, the force on a charge, and the motion of a charge.

Prior Knowledge: None
Instructors: Dr. Peter Dourmashkin, Prof. Gunther Roland
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