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Video Clips

RealVideo®
9:20 minutes (41:41 - 51:01)
Explanation of how a Van de Graaff generator works, with a demonstration of making one manually.
None
Prof. Walter Lewin
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RealVideo®
6:01 minutes (44:02 - 50:03)
A power supply generated from falling water. Not explained until a later lecture.
None
Prof. Walter Lewin
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RealVideo®
4:48 minutes (20:33 - 25:21)
Electric field inside a conductor is always zero. Charge on a conductor is distributed on the surface. Example of positive charge placed on a heart-shaped conductor.
Conductors (7:15 of video lecture 1)
Prof. Walter Lewin
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RealVideo®
6:29 minutes (25:21 - 31:50)
Charge placed on a hollow conductor will be distributed only on the outside surface. Demonstration using a metal paint can showing that there is no electric field inside a charged hollow conductor. Electric shielding is defined.
Conductors (7:15 of video lecture 1, 20:33 of video lecture 5)
Prof. Walter Lewin
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RealVideo®
4:38 minutes (31:50 - 36:28)
No electric field inside a hollow conductor that is placed in an electric field. Electric shielding and the Faraday cage are defined.
Conductors (7:15 of video lecture 1, 20:33 of video lecture 5)
Prof. Walter Lewin
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RealVideo®
6:05 minutes (37:07 - 43:12)
If charge placed inside a hollow conductor, there will be an opposite charge distributed on inside surface and an equal charge on the outside surface of the conductor.
Conductors (7:15 of video lecture 1, 20:33 of video lecture 5)
Prof. Walter Lewin
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RealVideo®
6:46 minutes (43:12 - 49:58)
Using a paint can to show that a hollow conductor in an electric field has charge distributed on the outside but no charge on the inside surface. Bringing a radio into a giant Faraday cage to demonstrate electric shielding. Getting inside a charged Faraday cage to show there is no charge on the inside surface.
Conductors (7:15 of video lecture 1, 20:33 of video lecture 5)
Prof. Walter Lewin
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RealVideo®
6:29 minutes (0:00 - 6:29)
Finding the charge density and electric field for conductors that are not completely symmetric.
Conductors (7:15 of video lecture 1, 20:33 of video lecture 5)
Prof. Walter Lewin
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RealVideo®
2:36 minutes (6:29 - 9:05)
Charging up a metal cooking pot to show that there is higher charge density where the curvature is greater on a conductor.
Conductors (7:15 of video lecture 1, 20:33 of video lecture 5)
Prof. Walter Lewin
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RealVideo®
8:03 minutes (27:24 - 35:27)
How ionized water and gravity generate the large potential differences in the Kelvin Water Dropper.
Kelvin Water Dropper (44:02 of video lecture 10)
Prof. Walter Lewin
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RealVideo®
11:51 minutes (35:27 - 47:18)
Repositioning the components of the Kelvin Water Dropper to demonstrate other interesting behavior.
Kelvin Water Dropper (44:02 of video lecture 10)
Prof. Walter Lewin
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Lecture Notes

PDF - 1 MB
Page 4 to page 14
Definition with examples. Electric field is zero inside a conductor; conductors are equipotential objects. Equipotential defined; electric field lines perpendicular to equipotentials. Link to visualization of conductor with a net positive charge in equilibrium.
Electric Fields (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 - 1 MB
Page 15 to page 17
Link to visualization of electrostatic force.
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 11
Effects of placing charge inside or outside a hollow conductor, with diagrams and a link to a visualization on inductive charging.
Conductors (pages 4-14 of Presentation 7)
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 diagrams and equations. Equations for energy stored in a capacitor.
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 1
Definition of shielding due to a hollow conductor, including a diagram and the definition of Faraday cage.
Conductors (R7)
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 8 to page 13
Conductors and insulators defined; e-fields inside conductors; uniqueness theorem and potential inside cavities.
Poisson's equation
Prof. Gabriella Sciolla
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Online Textbook Chapter

PDF
Page 15 to page 24
Gauss's Law applied to conductors to show E = 0 inside, E_t = 0, surface is equipotential; charge in cavity; charge on connected spheres; force on conductors.
Gauss's Law, 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 1
3-part Gauss's law problem; determining qualitative charge distributions for different locations of the charge.
Prof. Walter Lewin
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PDF
Problem 5
Calculating current, charge, capacitance delivered to Van de Graaff generator.
Prof. Walter Lewin
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PDF
Problem 1
Explaining creation of sparks in the apparatus.
Prof. Walter Lewin
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PDF
Problem 2
Drawing and explaining electric field near ellipsoid conductor.
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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Exam Questions

PDF
Problem 2
Explaining charged object interaction with uncharged conductors and insulators.
Dr. Peter Dourmashkin, Prof. Gunther Roland
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Java Applets

Java Applet
Requires Java Virtual Machine
Applet demonstrating a method for charging a conductor without ever making direct contact.
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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Java Applet
Requires Java Virtual Machine
Applet simulating the behavior of charges in a charged conducting slab.
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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