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Video Clips

RealVideo®
5:16 minutes (0:00 - 5:16)
Definition, with examples of electric field around a positive charge and a negative charge.
Electric Force, Coulomb's Law (29:30 of video lecture 1)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2), Electric Force (29:30 of video lecture 1)
Prof. Walter Lewin
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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.
Dipoles (22:28 of video lecture 2), Electroscopes (42:00 of video lecture 1)
Prof. Walter Lewin
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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.
Dipoles (22:28 of video lecture 2), Electric Field (beginning of video lecture 2)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2)
Prof. Walter Lewin
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RealVideo®
3:49 minutes (7:14 - 11:03)
Definition, work per unit charge to move from infinity to a specific location. Measured in volts.
Electric Field (beginning of video lecture 2) and Electrostatic Potential Energy (beginning of video lecture 4)
Prof. Walter Lewin
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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.
Electric Potential (7:14 of video lecture 4)
Prof. Walter Lewin
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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.
Electric Potential (7:14 of video lecture 4)
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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.
Electric Potential (7:14 of video lecture 4)
Prof. Walter Lewin
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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.
Electric Potential (7:14 of video lecture 4)
Prof. Walter Lewin
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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.
Electric Potential (7:14 of video lecture 4)
Prof. Walter Lewin
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RealVideo®
6:00 minutes (0:00 - 6:00)
Relationship between electric field and electric potential.
Electric Field (beginning of video lecture 2) and Electric Potential (7:14 of video lecture 4)
Prof. Walter Lewin
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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.
Electric Field (beginning of video lecture 2) and Electric Potential (7:14 of video lecture 4)
Prof. Walter Lewin
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RealVideo®
4:08 minutes (9:37 - 13:45)
Finding potential from the components of the electric field. Gradient is defined.
Electric Field (beginning of video lecture 2) and Electric Potential (7:14 of video lecture 4)
Prof. Walter Lewin
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RealVideo®
6:48 minutes (13:45 - 20:33)
Finding the electric field when potential is (10^5)*x in the x direction.
Electric Field (beginning of video lecture 2) and Electric Potential (7:14 of video lecture 4)
Prof. Walter Lewin
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RealVideo®
5:08 minutes (44:27 - 49:35)
Finding the increase in kinetic energy when an electron is moved across a potential difference.
Kinetic Energy (from 8.01)
Prof. Walter Lewin
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RealVideo®
8:53 minutes (3:00 - 11:53)
How changing potentials in heart cells keep the heart pumping.
None
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RealVideo®
8:37 minutes (11:53 - 20:30)
Electrocardiograms, defibrillators, and pacemakers are explained, including a demonstration of an electrocardiogram on a student.
How Your Heart Works Pt. 1 (3:00 of video lecture 19)
Prof. Walter Lewin
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Lecture Notes

PDF
Page 51 to page 54
Definition, with link to a visualization.
Fields and Coulomb's Law (pages 26-50 from presentation 1)
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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PDF
Page 1 to page 7
Comparison of gravitational and electric fields. Electric field lines defined with diagrams. Example problem without solution.
Electric Charge and Field (pages 45-54 from presentation 1)
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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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.
Gravitational Potential and Potential Energy (pages 10-16 of presentation 4)
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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PDF
Page 29 to page 32
Derivation of electric field as the gradient of potential
Electric Potential (pages 17-28 of presentation 4) and Electric Field (pages 45-54 of presentation 1)
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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PDF
Page 33 to page 36
Energy required to bring charges from infinity into a specific arrangement. Examples for 2 and 3 point charges.
Electric Potential (pages 17-28 of presentation 4)
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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PDF
Page 1 to page 6
Relationship between electric field and electric potential for point charges.
Electric Potential (pages 17-36 of presentation 4)
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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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.
Electric Fields, Potential, and Gauss's Law (pages 1-41 of presentation 5)
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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PDF
#
Page 14 to page 18
Electric potential; Lorentz force and magnetic force; Biot-Savart Law; magnetic dipole moments
Material is from presentations 1-5 and 14-20.
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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PDF
#
Page 27 to page 32
Finding the electric field, electric potential, magnetic field, and field energy between the plates of a charging capacitor.
Gauss's Law (pages 7-22 of presentation 5) and Ampere's Law (pages 21-26 of presentation 18)
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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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.
None
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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PDF
Page 1 to page 2
Definitions, with equations. Superposition, charge densities, and unit vectors are also defined.
Fields (R1)
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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PDF
Page 1 to page 2
Definitions, with equations and properties.
Electric Charge and Field (R2)
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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PDF
Page 4 to page 7
Definition; field lines; fields for ring and disk of charge.
Coulomb's Law
Prof. Gabriella Sciolla
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Online Textbook Chapters

PDF
Page 16 to page 19
Showing fields through arrows, field lines, grass seeds, and iron filings; motion of fields.
Vector fields
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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PDF
Page 7 to page 11
Definition; fields for point charges and field lines; force from fields.
Coulomb's Law
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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PDF
Page 2 to page 6
Definition; gravitational work and conservative forces; potential and potential energy for gravity.
Electric fields
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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PDF
Page 6 to page 10
Defined for E-fields and calculated for point charges and continuous distributions.
Work and potential
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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PDF
Page 10 to page 13
Deriving E-field from potential; equipotential surfaces defined.
Electric potential
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

PDF
Problem 16 to problem 17
Question about the electric field for two unequal point charges with opposite signs, with answer and explanation.
None
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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PDF
Problem 1 to problem 4
Two questions with answers and explanations.
None
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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PDF
Problem 5 to problem 8
Two questions with answers and explanations.
None
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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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.
None
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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PDF
Problem 1 to problem 2
Question with answer and explanation.
None
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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PDF
Problem 3 to problem 12
Five questions with answers and explanations.
None
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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PDF
Problem 7 to problem 10
Two questions about determining the electric field when the electric potential is known, with answers and explanations.
None
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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PDF
Problem 1 to problem 2
Question about walking down a mountain most quickly, with answer and explanation.
None
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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PDF
Problem 2
3-part E-field problem; calculating and plotting E-field along x-axis.
Prof. Walter Lewin
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PDF
Problem 2
3-part Gauss's law problem; finding radial E-field and potential.
Prof. Walter Lewin
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PDF
Problem 4
6-part point charge problem; e-fields and potentials from point charge distribution; potential and kinetic energy.
Prof. Walter Lewin
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PDF
Problem 6
4-part voltage problem; finding radius and voltage of charged sphere.
Prof. Walter Lewin
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PDF
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Problem 3
Finding position for third charge to cancel second; reaction to perturbation.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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PDF
Problem 3
Finding F and τ on dipole from E-field; charge of point from motion of dipole; acceleration from point charge force.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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PDF
Problem 1
Comparing potential and potential energy of opposite charges near a fixed point charge.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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PDF
Problem 2
Calculating initial speed of proton given distance traveled to nucleus.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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PDF
Problem 3
Explaining equipotentiality; comparing E-fields near spheres.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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PDF
Problem 1
4-part problem; finding force on one charge, E-field along x-axis and y-axis, graphing, and drawing field lines.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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PDF
Problem 2
Graphing and approximating electric potential; graphing potential energy.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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Exam Questions

PDF
Problem 3
Finding field lines for E-field with given effect on dipole; F and τ on dipole for greater negative charge.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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PDF
Problem 1
For triangular arrangement of charges, finding the E-field, the force on a charge, and the motion of a charge.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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