MIT educated Dr. Radi Jishi continues with Advanced Placement Physics C (Electricity and Magnetism). AP Physics C is Calculus based and Dr. Jishi makes sure each student fully understands the more complicated mathematics. College students will find the course equally as helpful as high school students planning to ace the Advanced Placement test since the course offers detailed explanations and plenty of comprehensive extra examples.
| I. Electricity |
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Electric Force |
56:18 |
| | |
Intro |
0:00 | |
| | |
Electric Charge |
0:18 | |
| | |
| Matter Consists of Atom |
1:01 | |
| | |
| Two Types of Particles: Protons & Neutrons |
1:48 | |
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| Object with Excess Electrons: Negatively Charged |
7:58 | |
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| Carbon Atom |
8:30 | |
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| Positively Charged Object |
9:55 | |
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Electric Charge |
10:07 | |
| | |
| Rubber Rod Rubs Against Fur (Negative Charge) |
10:16 | |
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| Glass Rod Rub Against Silk (Positive Charge) |
11:48 | |
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| Hanging Rubber Rod |
12:44 | |
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Conductors and Insulators |
16:00 | |
| | |
| Electrons Close to Nucleus |
18:34 | |
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| Conductors Have Mobile Charge |
21:30 | |
| | |
| Insulators: No Moving Electrons |
23:06 | |
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| Copper Wire Connected to Excess Negative charge |
23:22 | |
| | |
| Other End Connected to Excess Positive Charge |
24:09 | |
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Charging a Metal Object |
27:25 | |
| | |
| By Contact |
28:05 | |
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| Metal Sphere on an Insulating Stand |
28:16 | |
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| Charging by Induction |
30:59 | |
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| Negative Rubber Rod |
31:26 | |
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| Size of Atom |
36:08 | |
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Extra Example 1: Three Metallic Objects |
7:32 | |
| | |
Extra Example 2: Rubber Rod and Two Metal Spheres |
6:25 | |
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Coulomb's Law |
87:18 |
| | |
Intro |
0:00 | |
| | |
Coulomb's Law |
0:59 | |
| | |
| Two Point Charges by Distance R |
1:11 | |
| | |
| Permitivity of Free Space |
5:28 | |
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Charges on the Vertices of a Triangle |
8:00 | |
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| 3 Charges on Vertices of Right Triangle |
8:29 | |
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| Charge of 4, -5 and -2 micro-Coulombs |
10:00 | |
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| Force Acting on Each Charge |
10:58 | |
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Charges on a Line |
21:29 | |
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| 2 Charges on X-Axis |
22:40 | |
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| Where Should Q should be Placed, Net Force =0 |
23:23 | |
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Two Small Spheres Attached to String |
31:08 | |
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| Adding Some Charge |
32:03 | |
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| Equilibrium Net Force on Each Sphere = 0 |
33:38 | |
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Simple Harmonic Motion of Point Charge |
37:40 | |
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| Two Charges on Y-Axis |
37:55 | |
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| Charge is Attracted |
39:52 | |
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| Magnitude of Net Force on Q |
42:23 | |
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Extra Example 1: Vertices of Triangle |
9:39 | |
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Extra Example 2: Tension in String |
11:46 | |
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Extra Example 3: Two Conducting Spheres |
6:29 | |
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Extra Example 4: Force on Charge |
9:21 | |
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Electric Field |
97:24 |
| | |
Intro |
0:00 | |
| | |
Definition of Electric Field |
0:11 | |
| | |
| Q1 Produces Electric Field |
3:23 | |
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| Charges on a Conductor |
4:26 | |
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Field of a Point Charge |
13:10 | |
| | |
| Charge Point Between Two Fields |
13:20 | |
| | |
| Electric Field E=kq/r2 |
14:29 | |
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| Direction of the Charge Field |
15:10 | |
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| Positive Charge, Field is Radially Out |
15:45 | |
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Field of a Collection of a Point Charge |
19:40 | |
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| Two Charges Q1,Q2 |
19:56 | |
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| Q1 Positive, Electric Field is Radially Out |
20:32 | |
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| Q2 is Negative, Electric Field is Radially Inward |
20:46 | |
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| 4 Charges are Equal |
23:54 | |
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Parallel Plate Capacitor |
25:42 | |
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| Two Plates ,Separated by a Distance |
26:44 | |
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| Fringe Effect |
30:26 | |
| | |
| E=Constant Between the Parallel Plate Capacitor |
30:40 | |
| | |
Electric Field Lines |
35:16 | |
| | |
| Pictorial Representation of Electric Field |
35:30 | |
| | |
| Electric Lines are Tangent to the Vector |
35:57 | |
| | |
| Lines Start at Positive Charge, End on Negative Charge |
41:24 | |
| | |
| Parallel Line Proportional to Charge |
45:51 | |
| | |
| Lines Never Cross |
46:00 | |
| | |
Conductors and Shielding |
49:33 | |
| | |
| Static Equilibrium |
51:09 | |
| | |
| No Net Moment of Charge |
53:09 | |
| | |
| Electric Field is Perpendicular to the Surface of Conductor |
55:40 | |
| | |
Extra Example 1: Plastic Sphere Between Capacitor |
8:46 | |
| | |
Extra Example 2: Electron Between Capacitor |
11:52 | |
| | |
Extra Example 3: Zero Electric Field |
10:44 | |
| | |
Extra Example 4: Dimensional Analysis |
6:01 | |
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Electric Field of a Continuous Charge Distribution |
100:12 |
| | |
Intro |
0:00 | |
| | |
General Expression For E |
0:16 | |
| | |
| Magnitude of Electric Field |
1:29 | |
| | |
| Disk: Spread Charge Distribution |
5:04 | |
| | |
| Volume Contains Charges |
6:16 | |
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Charged Rod One Dimension |
16:28 | |
| | |
| Rod in X-Axis |
17:00 | |
| | |
| Charge Density |
17:49 | |
| | |
| Find Electric Field at Distance 'A' |
19:05 | |
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Charged Rod, Cont. |
32:48 | |
| | |
| Origin at Center, Extends From -L to +L |
33:11 | |
| | |
| Dividing Rod into Pieces |
34:50 | |
| | |
| Electric Field Produced At Point P |
35:09 | |
| | |
| Another Element |
37:43 | |
| | |
| 'Y' Components of Electric Field |
42:15 | |
| | |
Charged Ring |
54:23 | |
| | |
| Find Electric Field Above the Center |
54:48 | |
| | |
Charged Disc |
58:43 | |
| | |
| Collection of Rings |
59:10 | |
| | |
Example 1: Charged Disk |
17:18 | |
| | |
Example 2: Semicircle with Charge |
7:49 | |
| | |
Example 3: Charged Cylindrical Charge |
13:53 | |
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Gauss's Law |
87:00 |
| | |
Intro |
0:00 | |
| | |
Electric Field Lines |
0:11 | |
| | |
| Magnitude of Field |
2:04 | |
| | |
| Unit Area and Unit Lines |
2:59 | |
| | |
| Number of Lines Passing Through the Unit |
6:45 | |
| | |
Electic Flux: Constant E |
6:51 | |
| | |
| Field Lines Equally Spaced |
7:10 | |
| | |
| Area Perpendicular To Field Lines |
7:46 | |
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| Electric Flux |
8:36 | |
| | |
| Area Perpendicular to Electric Lines |
9:43 | |
| | |
| Tilt the Area |
10:58 | |
| | |
| Flux of E Through Area |
17:30 | |
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Electric Flux: General Case |
20:46 | |
| | |
| Perpendicular at Different Directions |
23:24 | |
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| Electric Field Given On a Patch |
27:10 | |
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| Magnitude of Field |
28:53 | |
| | |
| Direction is Outward Normal |
29:34 | |
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| Flux Through Patch |
30:36 | |
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Example |
36:09 | |
| | |
| Electric Field in Whole Space |
37:16 | |
| | |
| Sphere of Radius 'r' |
37:30 | |
| | |
| Flux Through Sphere |
38:09 | |
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Gauss's Law: Charge Outside |
46:02 | |
| | |
| Flux Through Radius Phase is Zero |
50:09 | |
| | |
| Outward normal 'n' |
54:55 | |
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Gauss's Law: Charge Enclosed |
60:30 | |
| | |
| Drawing Cones |
60:51 | |
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Example 1: Flux Through Square |
7:08 | |
| | |
Example 2: Flux Through Cube |
10:23 | |
| | |
Example 3: Flux Through Pyramid |
5:01 | |
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Application of Gauss's Law, Part 1 |
66:48 |
| | |
Intro |
0:00 | |
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When is Gauss Law Useful? |
0:18 | |
| | |
| Need a Surface S |
5:14 | |
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| Gaussian Surface |
5:50 | |
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Sphere of Charge |
10:11 | |
| | |
| Charge Density is Uniform |
10:30 | |
| | |
| Radius as 'A' |
11:23 | |
| | |
| Case 1: R>A |
11:58 | |
| | |
| Any Direction On Cone Is Same |
20:28 | |
| | |
| Case 2: R<A |
25:15 | |
| | |
| Point R Within the Surface |
25:30 | |
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Concentric Cavity |
31:11 | |
| | |
| Inside Circle and Outside Circle |
31:48 | |
| | |
| R>A |
32:17 | |
| | |
| R<B |
36:40 | |
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Radius Dependent Charge Density |
37:39 | |
| | |
| Sphere |
38:09 | |
| | |
| Total Charge: Q |
39:46 | |
| | |
| Spherical Shell |
40:13 | |
| | |
| Finding Electric Field R>A |
42:36 | |
| | |
| R<A |
44:14 | |
| | |
Example 1: Charged Sphere |
9:56 | |
| | |
Example 2: Charged Spherical Cavity |
11:06 | |
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Application of Gauss's Law, Part 2 |
79:19 |
| | |
Intro |
0:00 | |
| | |
Infinitely Long Line of Charge |
0:13 | |
| | |
| All Points Same Magnitude |
5:02 | |
| | |
| E is Perpendicular to Line |
9:08 | |
| | |
| Gauss's Law Cannot be Applied to Finite Length |
15:50 | |
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Infinitely Long Cylinder Of Charge |
16:05 | |
| | |
| Draw a Cylinder of Radius 'R' |
16:36 | |
| | |
| Line of Charge Along the Center |
18:25 | |
| | |
| R<A |
18:39 | |
| | |
| Electric Field of Special Direction |
19:06 | |
| | |
Infinite Sheet of Charge |
25:12 | |
| | |
| Electric Field Above the Sheet |
25:38 | |
| | |
| Point is Above Height, Cylinder Intersects |
26:29 | |
| | |
| Curved Path |
33:12 | |
| | |
Parallel Plate Capacitors |
37:16 | |
| | |
| Electric Field Between Sheets |
39:16 | |
| | |
Conductors |
41:55 | |
| | |
| Adding Charge to Conductors |
42:16 | |
| | |
| In Electrostatic Equilibrium Charges Stop Moving |
44:37 | |
| | |
| Electric Field is Perpendicular to Surface |
47:16 | |
| | |
| Excess Charge Must Reside on Surface |
47:38 | |
| | |
Example 1: Cylindrical Shell |
7:45 | |
| | |
Example 2: Wire Surrounded by Shell |
6:43 | |
| | |
Example 3: Sphere Surrounded by Spherical Shell |
7:30 | |
| |
Electric Potential, Part 1 |
86:57 |
| | |
Intro |
0:00 | |
| | |
Potential Difference Between Two Points |
0:16 | |
| | |
| Electric Field in Space By Stationary Charges |
0:30 | |
| | |
| Point Charge Moves From A to B |
1:37 | |
| | |
| Electric Field Exerts a Force |
1:50 | |
| | |
| Electric Potential Energy |
5:34 | |
| | |
| Work Done By External Agent |
20:03 | |
| | |
| Change in Potential Energy is Equal to Amount of Work Done |
24:06 | |
| | |
Potential Difference in Uniform Electric Field |
27:59 | |
| | |
| Constant Electric Field |
28:22 | |
| | |
| Equipotential |
40:22 | |
| | |
Parallel Plates |
40:52 | |
| | |
| Electric Field is Perpendicular to Plate |
42:07 | |
| | |
| Charge Released at A from Rest |
49:00 | |
| | |
Motion of Charged Particle in a Uniform Electric Field |
51:55 | |
| | |
Example 1: Work by Moving Electrons |
3:45 | |
| | |
Example 2: Block and Spring |
13:52 | |
| | |
Example 3: Particle on String |
11:27 | |
| |
Electric Potential, Part 2 |
91:50 |
| | |
Intro |
0:00 | |
| | |
Potential of a Point Charge |
0:32 | |
| | |
| Potential Difference Between A to B |
1:25 | |
| | |
| Draw a Circle |
9:12 | |
| | |
| Tangential to Sphere |
9:33 | |
| | |
| Moving Normally From Sphere |
12:33 | |
| | |
Potential Energy of a Collection of Charges |
26:33 | |
| | |
| Potential Energy of Two Charges |
26:44 | |
| | |
| Work Done in Assembling the Configuration |
27:29 | |
| | |
| Bringing From Infinity to New Location |
33:57 | |
| | |
| Work Done by External Agent |
36:22 | |
| | |
| Potential Energy of the System |
39:39 | |
| | |
| Potential Energy for Two Charges |
40:00 | |
| | |
Example |
44:49 | |
| | |
| Two Charges |
45:03 | |
| | |
| Speed at Infinity |
48:01 | |
| | |
Electric Field from the Potential |
51:12 | |
| | |
| Finding E if V is Given |
51:33 | |
| | |
Electric Dipole |
56:22 | |
| | |
| Two Equal and Opposite Charges Separated By a Distance |
56:32 | |
| | |
| If a << r1 or r2 |
60:23 | |
| | |
Example 1: Two Point Charges |
17:56 | |
| | |
Example 2: Two Insulating Spheres |
7:31 | |
| | |
Example 3: Electric Potential of Space |
4:01 | |
| |
Electric Potential, Part 3 |
69:12 |
| | |
Intro |
0:00 | |
| | |
| Continuous Charge Distribution |
0:27 | |
| | |
| Finding Potential for a Charge Point |
1:39 | |
| | |
| Potential Produced at P |
4:42 | |
| | |
Charged Ring |
8:38 | |
| | |
| Electric Field at Some Point of Axis |
9:13 | |
| | |
Charged Disk |
19:32 | |
| | |
| Collection of Ring |
20:40 | |
| | |
| Finding Potential Point Above the Ring |
22:19 | |
| | |
| Potential Due to The Ring |
23:40 | |
| | |
Finite Line of Charge |
35:56 | |
| | |
| Line of Change Along the X-Axis and Y-axis |
36:11 | |
| | |
Example 1: Charged Rod |
8:52 | |
| | |
Example 2: Bent Semicircle |
4:48 | |
| | |
Example 3: Bent Semicircle with Variables |
4:52 | |
| |
Electric Potential, Part 4 |
71:16 |
| | |
Intro |
0:00 | |
| | |
Charged Conductors |
0:12 | |
| | |
| Adding Excess Charge to a Conductor |
1:02 | |
| | |
| E=0 Inside Conductors |
1:50 | |
| | |
| Excess Charges Must Reside on Surface |
3:40 | |
| | |
| E Normal on the Surface |
9:31 | |
| | |
| Surface of Conductor is Equipotential |
11:59 | |
| | |
Conducting Sphere |
19:28 | |
| | |
| Adding Charge to the Sphere |
19:41 | |
| | |
| Electric Field Outside is Concentrated at Center |
20:05 | |
| | |
| Electric Potential is Same as Center |
23:01 | |
| | |
Example |
26:24 | |
| | |
| Two Spheres with Distance and of Different Size |
26:45 | |
| | |
| Connecting Both Spheres with Conducting Wire |
27:22 | |
| | |
Cavity Within a Conductor |
39:43 | |
| | |
| Hollow Conductor |
40:19 | |
| | |
| Electric Static Equilibrium |
41:13 | |
| | |
| Electric Field is Zero Within Cavity |
53:20 | |
| | |
Example 1: Neutral Conducting Sphere |
4:03 | |
| | |
Example 2: Conducting Sphere with Spherical Shell |
13:45 | |
| |
Capacitor |
84:14 |
| | |
Intro |
0:00 | |
| | |
Capacitance |
0:09 | |
| | |
| Consider Two Conductor s |
0:25 | |
| | |
| Electric Field Passing from Positive to Negative |
1:19 | |
| | |
| Potential Difference |
3:31 | |
| | |
| Defining Capacitance |
3:51 | |
| | |
Parallel Plate Capacitance |
8:30 | |
| | |
| Two Metallic Plates of Area 'a' and Distance 'd' |
8:46 | |
| | |
| Potential Difference between Plates |
13:12 | |
| | |
Capacitance with a Dielectric |
22:14 | |
| | |
| Applying Electric Field to a Capacitor |
22:44 | |
| | |
| Dielectric |
30:32 | |
| | |
Example |
34:56 | |
| | |
| Empty Capacitor |
35:12 | |
| | |
| Connecting Capacitor to a Battery |
35:26 | |
| | |
| Inserting Dielectric Between Plates |
39:02 | |
| | |
Energy of a Charged Capacitor |
43:01 | |
| | |
| Work Done in Moving a Charge, Difference in Potential |
47:48 | |
| | |
Example |
54:10 | |
| | |
| Parallel Plate Capacitor |
54:22 | |
| | |
| Connect and Disconnect the Battery |
55:27 | |
| | |
| Calculating Q=cv |
55:50 | |
| | |
| Withdraw Mica Sheet |
56:49 | |
| | |
| Word Done in Withdrawing the Mica |
60:23 | |
| | |
Extra Example 1: Parallel Plate Capacitor |
8:41 | |
| | |
Extra Example 2: Mica Dielectric |
15:01 | |
| |
Combination of Capacitors |
63:23 |
| | |
Intro |
0:00 | |
| | |
Parallel Combination |
0:20 | |
| | |
| Two Capacitors in Parallel With a Battery |
0:40 | |
| | |
| Electric Field is Outside |
5:47 | |
| | |
| Point A is Directly Connected to Positive Terminal |
7:57 | |
| | |
| Point B is Directly Connected to Negative Terminal |
8:10 | |
| | |
| Voltage Across Capacitor |
12:54 | |
| | |
| Energy Stored |
14:52 | |
| | |
Series Combination |
17:58 | |
| | |
| Two Capacitors Connected End to End With a Battery |
18:10 | |
| | |
| Equivalent Capacitor |
25:20 | |
| | |
| A is Same Potential |
26:59 | |
| | |
| C is Same Potential |
27:06 | |
| | |
| Potential Difference Across First Capacitor (Va-Vb) |
27:42 | |
| | |
| (Vb-Vc) is Potential Difference Across Second Capacitor |
28:10 | |
| | |
| Energy Stored in C1,C2 |
29:53 | |
| | |
Example |
31:07 | |
| | |
| Two Capacitor in Series, 2 in Parallel, 3 in Parallel, 1 Capacitor Connected |
31:28 | |
| | |
| Final Equivalent Circuit |
37:31 | |
| | |
Extra Example 1: Four Capacitors |
16:50 | |
| | |
Extra Example 2: Circuit with Switches |
8:25 | |
| |
Calculating Capacitance |
55:14 |
| | |
Intro |
0:00 | |
| | |
Considering a Sphere |
0:28 | |
| | |
| Placing Charge on Sphere |
2:14 | |
| | |
| On the Surface of Sphere |
4:12 | |
| | |
Spherical Capacitor |
9:20 | |
| | |
| Sphere of Radius a and Shell of Radius b |
9:40 | |
| | |
| Positive Charge on Outer Sphere |
11:02 | |
| | |
| Negative Charge on Inner Sphere |
11:26 | |
| | |
| Calculating Potential Difference |
11:38 | |
| | |
Parallel Plate Capacitor |
22:38 | |
| | |
| Two Plates with Charges Positive and Negative |
22:54 | |
| | |
| Separation of Plate |
25:10 | |
| | |
Cylindrical Capacitor |
28:40 | |
| | |
| Inner Cylinder and Outer Cylindrical Shell |
29:01 | |
| | |
| Linear Charge Density |
30:41 | |
| | |
Example 1: Parallel Plate Capacitor |
4:39 | |
| | |
Example 2: Spherical Capacitor |
8:51 | |
| |
More on Filled Capacitors |
77:13 |
| | |
Intro |
0:00 | |
| | |
Electric Dipole is an Electric Field : Torque |
0:13 | |
| | |
| Magnitude of Dipole |
1:15 | |
| | |
| Starts to Rotate |
5:38 | |
| | |
| Force qe to the Right |
5:59 | |
| | |
| Finding the Torque |
6:35 | |
| | |
Electric Dipole is an Electric Field : Potential Energy |
13:56 | |
| | |
| Electric Field Try's to Rotate |
14:43 | |
| | |
| Object on Center of Earth |
16:04 | |
| | |
| Applying Torque Equal and Opposite |
17:05 | |
| | |
Water Molecule |
25:43 | |
| | |
| Carbon Molecules |
31:39 | |
| | |
| Net Dipole Moment is Zero |
32:11 | |
| | |
| Induced Dipole Moment |
34:43 | |
| | |
Filled Capacitor |
35:27 | |
| | |
| Empty Capacitor with Charge on it |
35:44 | |
| | |
| Inserting a Dielectric |
36:08 | |
| | |
Capacitor Partially Filled with Metallic Slab |
44:33 | |
| | |
| Capacitor with Slab of Distance 'd' |
44:54 | |
| | |
Capacitor Partially Filled with a Dielectric Slab |
51:59 | |
| | |
| Change in Potential Difference |
53:28 | |
| | |
Example 1: Parallel Plate Capacitor |
13:37 | |
| | |
Example 2: Conducting Slab |
8:20 | |
| |
Electric Current |
79:17 |
| | |
Intro |
0:00 | |
| | |
Definition |
0:20 | |
| | |
| Consider a Wire ,Cylindrical |
0:40 | |
| | |
| Cross Sectional Area |
1:06 | |
| | |
| Crossing Charges Will be Counted |
2:50 | |
| | |
| Amount of Charge Crosses Cross Sectional Area |
3:29 | |
| | |
| Current I=q/t |
4:18 | |
| | |
| Charges Flowing in Opposite Direction |
5:58 | |
| | |
| Current Density |
6:19 | |
| | |
| Applying Electric Field |
11:50 | |
| | |
Current in a Wire |
15:24 | |
| | |
| Wire With a Cross Section Area 'A' |
15:33 | |
| | |
| Current Flowing to Right |
18:57 | |
| | |
| How Much Charge Crosses Area 'A' |
19:15 | |
| | |
| Drift Velocity |
20:02 | |
| | |
| Carriers in Cylinder |
22:40 | |
| | |
Ohm's Law |
24:58 | |
| | |
| Va-Vb = Electric Field times Length of Wire |
28:27 | |
| | |
| Ohm's Law |
28:54 | |
| | |
| Consider a Copper Wire of 1m , Cross Sectional Area 1cm/sq |
34:24 | |
| | |
Temperature Effect |
37:07 | |
| | |
| Heating a Wire |
37:05 | |
| | |
| Temperature Co-Efficient of Resistivity |
39:57 | |
| | |
Battery EMF |
43:00 | |
| | |
| Connecting a Resistance to Battery |
44:30 | |
| | |
| Potential Difference at Terminal of Battery |
45:15 | |
| | |
Power |
53:30 | |
| | |
| Battery Connected with a Resistance |
53:47 | |
| | |
| Work Done on Charge |
56:55 | |
| | |
| Energy Lost Per Second |
60:35 | |
| | |
Extra Example 1: Current |
9:46 | |
| | |
Extra Example 2: Water Heater |
8:05 | |
| |
Circuits |
94:08 |
| | |
Intro |
0:00 | |
| | |
Simple Rules |
0:16 | |
| | |
| Resistance in Series |
0:33 | |
| | |
| Current Passing Per Second is Equal |
1:36 | |
| | |
| Potential Difference |
3:10 | |
| | |
| Parallel Circuit, R1, R2 |
5:08 | |
| | |
| Battery, Current Starts From Positive Terminal to Negative Terminal |
10:08 | |
| | |
Series Combination of Resistances |
13:06 | |
| | |
| R1, R2 Connected to Battery |
13:35 | |
| | |
| Va-Vb=Ir1,Vb-Vc=Ir2 |
16:59 | |
| | |
| Three Resistance Connected in Series Req=r1+r2+r3 |
18:55 | |
| | |
Parallel Combination of Resistance |
19:28 | |
| | |
| R1 and R2 Combined Parallel |
19:50 | |
| | |
| I=i1+i2 (Total Current) |
24:26 | |
| | |
| Requ=I/E |
24:51 | |
| | |
A Simple Circuit |
27:57 | |
| | |
| Current Splits |
29:15 | |
| | |
| Total Resistance |
31:52 | |
| | |
| Current I= 6/17.2 |
35:10 | |
| | |
Another Simple Circuit |
37:46 | |
| | |
| Battery has Small Internal Resistance |
38:02 | |
| | |
| 2 Ohms Internal Resistance, and Two Resistance in Parallel |
38:24 | |
| | |
| Drawing Circuit |
48:53 | |
| | |
| Finding Current |
52:06 | |
| | |
RC Circuit |
55:17 | |
| | |
| Battery , Resistance and Capacitance Connected |
55:30 | |
| | |
| Current is Function of Time |
58:00 | |
| | |
| R, C are Time Constants |
59:25 | |
| | |
Extra Example 1: Resistor Current/Power |
4:17 | |
| | |
Extra Example 2: Find Current |
6:03 | |
| | |
Extra Example 3: Find Current |
10:00 | |
| | |
Extra Example 4: Find Current |
13:49 | |
| |
Kirchhoff's Law |
102:02 |
| | |
Intro |
0:00 | |
| | |
First Kirchhoff Rule |
0:19 | |
| | |
| Two Resistance Connected With a Battery |
0:29 | |
| | |
| Many Resistance |
1:40 | |
| | |
| Increase in Potential from A to B |
4:46 | |
| | |
| Charge Flowing from Higher Potential to Lower Potential |
5:13 | |
| | |
Second Kirchhoff Rule |
9:17 | |
| | |
| Current Entering |
9:27 | |
| | |
| Total Current Arriving is Equal Current Leaving |
13:20 | |
| | |
Example |
14:10 | |
| | |
| Battery 6 V, Resistance 20, 30 Ohms and Another Battery 4v |
14:30 | |
| | |
| Current Entering I2+I3 |
21:18 | |
| | |
Example 2 |
31:20 | |
| | |
| 2 Loop circuit with 6v and 12 v and Resistance, Find Current in Each Resistance |
32:29 | |
| | |
Example 3 |
42:02 | |
| | |
| Battery and Resistance in Loops |
42:23 | |
| | |
Ammeters and Voltmeters |
56:22 | |
| | |
| Measuring Current is Introducing an Ammeter |
56:35 | |
| | |
| Connecting Voltmeter, High Resistance |
57:31 | |
| | |
Extra Example 1: Find Current |
18:47 | |
| | |
Extra Example 2: Find Current |
13:35 | |
| | |
Extra Example 3: Find Current |
10:23 | |
| |
RC Circuits |
80:35 |
| | |
Intro |
0:00 | |
| | |
Charging a Capacitor: Circuit Equation |
0:09 | |
| | |
| Circuit with a Resistance , Capacitance and a Battery |
0:20 | |
| | |
| Closing Switch at T=0 |
1:36 | |
| | |
| Applying Kirchhoff's Rule |
6:26 | |
| | |
| Change in Potential is Zero |
6:52 | |
| | |
| Solution Tau dq/dt= ec-q |
16:25 | |
| | |
Discharging a Capacitor |
27:14 | |
| | |
| Charged Capacitor Connect to Switch and Resistance |
27:30 | |
| | |
| Closing the Switch at T=0 |
28:11 | |
| | |
Example |
36:50 | |
| | |
| 12V Battery with Switch and Resistance 10mili ohms and Capacitor Connected 10 Micro Farad |
37:02 | |
| | |
| Time Constant |
38:58 | |
| | |
| Charge at q=0 at t=1sec |
40:16 | |
| | |
Example |
42:58 | |
| | |
| Switch With Capacitor and Resistance |
43:31 | |
| | |
| What Time Charge C Has Initial Valve |
45:17 | |
| | |
| How Long Charge Energy Stored in C to Drop Half of Initial Value |
46:55 | |
| | |
Example 1: RC Circuit 1 |
6:49 | |
| | |
Example 2: RC Circuit 2 |
12:53 | |
| | |
Example 3: RC Circuit 3 |
10:42 | |
| II. Magnetism |
| |
Magnetic Field |
98:19 |
| | |
Intro |
0:00 | |
| | |
Magnets |
0:13 | |
| | |
| Compass Will Always Point North |
3:49 | |
| | |
| Moving a Compass Needle |
5:50 | |
| | |
Force on a Charged Particles |
10:37 | |
| | |
| Electric Field and Charge Particle Q |
10:48 | |
| | |
| Charge is Positive Force |
11:11 | |
| | |
| Charge Particle is At Rest |
13:38 | |
| | |
| Taking a Charged Particle and Moving to Right |
16:15 | |
| | |
| Using Right Hand Rule |
23:37 | |
| | |
| C= Magnitude of A, B |
26:30 | |
| | |
| Magnitude of C |
26:55 | |
| | |
Motion of Particle in Uniform Magnetic Field |
33:30 | |
| | |
| Magnetic Field has Same Direction |
34:02 | |
| | |
| Direction of Force |
38:40 | |
| | |
| Work Done By Force=0 |
41:40 | |
| | |
| Force is Perpendicular With Velocity |
42:00 | |
| | |
Bending an Electron Beam |
48:09 | |
| | |
| Heating a Filament |
48:29 | |
| | |
| Kinetic Energy of Battery |
51:54 | |
| | |
| Introducing Magnetic Field |
52:10 | |
| | |
Velocity Selector |
53:45 | |
| | |
| Selecting Particles of Specific Velocity |
54:00 | |
| | |
| Parallel Plate Capacitor |
54:30 | |
| | |
| Magnetic Force |
56:20 | |
| | |
| Magnitude of Force |
56:45 | |
| | |
Extra Example 1: Vectors |
19:24 | |
| | |
Extra Example 2: Proton in Magnetic Field |
8:33 | |
| | |
Extra Example 3: Proton Circular Path |
10:46 | |
| |
Magnetic Force on a Current Carrying Conductor |
64:43 |
| | |
Intro |
0:00 | |
| | |
Current Carrying Conductor in a Magnetic Field |
0:19 | |
| | |
| Current Though the Wire Connected to Battery |
1:22 | |
| | |
| Current Exerts Force Toward the Left |
2:16 | |
| | |
| IF Current is Reversed ,Force Exerts on Right |
2:47 | |
| | |
Magnetic Force |
3:31 | |
| | |
| Wire with Current 'I' and with magnetic Field |
4:02 | |
| | |
| Force Exerted by Magnetic field |
5:05 | |
| | |
| Applying right hand Rule |
5:25 | |
| | |
| Let N be Number of Charge Carries Per /Vol |
6:40 | |
| | |
| Force on Wire |
8:30 | |
| | |
| Number of Charge Crossing in Time 't' |
12:51 | |
| | |
Example |
22:32 | |
| | |
| Wire Bent to Semi Circle and Rest is Straight |
22:51 | |
| | |
| Applying Constant Magnetic Field in 'y' Direction |
23:24 | |
| | |
| Force n Straight Segment |
23:50 | |
| | |
| Net Force |
34:19 | |
| | |
Example 1: Rod on Rails |
15:37 | |
| | |
Example 2: Magnetic Force on Wire |
13:59 | |
| |
Torque on a Current Carrying Loop |
69:06 |
| | |
Intro |
0:00 | |
| | |
B-Field Parallel to Plane of the Loop |
0:27 | |
| | |
| Loop in the X-Y Plane |
1:06 | |
| | |
| Net Force on Loop |
7:45 | |
| | |
B-Field Not Parallel to Plane of the Loop |
15:16 | |
| | |
| Loop in the X-Y Plane, Free to Rotate in X- Direction |
15:32 | |
| | |
| Force on Out of Page and Force in to the Page |
15:59 | |
| | |
| Loop Turns Through 90 Degrees |
18:10 | |
| | |
Magnetic Moment |
36:26 | |
| | |
| Any Current Loop Has Current 'I' |
36:51 | |
| | |
| Electric Dipole in Electric Field |
38:17 | |
| | |
| Potential Energy |
39:54 | |
| | |
| Magnetic Potential Energy of Dipole |
41:05 | |
| | |
Example |
43:33 | |
| | |
| Circular of Radius 'r' With Magnetic Field and Pass Current |
43:42 | |
| | |
| Torque |
46:01 | |
| | |
Example 1: Loop in Magnetic Field |
9:21 | |
| | |
Example 2: Rotating Charge |
10:32 | |
| |
Magnetic Field Produced By Current, Part 1 |
57:58 |
| | |
Intro |
0:00 | |
| | |
Biot-Savart Law |
0:11 | |
| | |
| Suppose A current Carrying Wire |
0:50 | |
| | |
| Magnetic Field Produced by the Tiny Element is Also Tiny |
3:09 | |
| | |
| Permeability of Free Space |
4:56 | |
| | |
B-Field of a Straight Wire |
8:40 | |
| | |
| Wire in X Axis |
9:05 | |
| | |
| What is the Magnetic Field Produce at Point p |
9:16 | |
| | |
| Taking a Small Segment |
9:57 | |
| | |
| If Length is Infinite |
26:26 | |
| | |
Semi Circular Wire |
27:02 | |
| | |
| Semicircular Wire of Radius 'R' |
27:22 | |
| | |
| Finding Magnetic Field at Center |
27:48 | |
| | |
Circular Current in Loop |
33:37 | |
| | |
| Circular Loop with Current 'I' |
33:47 | |
| | |
| Current Above the Center |
34:00 | |
| | |
Example 1: Loop Carrying Current |
10:42 | |
| | |
Example 2: Concentric Loops |
4:57 | |
| |
Magnetic Field Produced By Current, Part 2 |
79:29 |
| | |
Intro |
0:00 | |
| | |
Ampere's Law |
0:16 | |
| | |
| Consider a Loop at Any Point in Loop |
1:15 | |
| | |
Long Cylindrical Wire |
9:08 | |
| | |
| Wire of Radius 'r' |
9:24 | |
| | |
| Magnetic Field is Tangent to Circle and Has Same Magnitude |
10:15 | |
| | |
| B at r>R |
21:58 | |
| | |
| B at r<R |
23:08 | |
| | |
| B at r=R |
25:49 | |
| | |
Toroid |
26:58 | |
| | |
| Wrap a Wire to Toroid |
27:47 | |
| | |
| Calculating the Magnetic Field for 1 Loop |
29:30 | |
| | |
Solenoid |
39:17 | |
| | |
| Coil With Many Turns |
39:35 | |
| | |
| Each Loop Carrying Current |
40:29 | |
| | |
| Taking Loop Within the Solenoid and Close the Loop |
43:05 | |
| | |
| Applying Ampere's Law |
43:33 | |
| | |
Example 1: Infinitely Long Wire |
8:12 | |
| | |
Example 2: Straight Wire |
4:15 | |
| | |
Example 3: Two Parallel Conductors |
8:21 | |
| | |
Example 4: Solenoid |
10:13 | |
| |
Magnetic Field Produced By Current, Part 3 |
50:37 |
| | |
Intro |
0:00 | |
| | |
Magnetic Force Between Parallel Conductors |
0:16 | |
| | |
| Two Parallel Plate Capacitors with Current |
0:40 | |
| | |
| Magnetic Field by i1 |
1:50 | |
| | |
| According to Right Hand Rule |
2:37 | |
| | |
Example |
10:20 | |
| | |
| Wire of 4m Length |
10:50 | |
| | |
| Mass of Wire 1Kg |
11:18 | |
| | |
| Force of Repulsion =Mg |
12:24 | |
| | |
Gauss's Law in Magnetism |
15:36 | |
| | |
| Surface of Area, Magnetic Field is Perpendicular to Surface |
17:09 | |
| | |
| Magnetic Flux Through Enclosed surface |
19:23 | |
| | |
Example |
26:44 | |
| | |
| Magnetic Field Out of Page |
27:54 | |
| | |
| Consider a Flux Through Rectangular Loop |
28:52 | |
| | |
Example 1: Two Parallel Wires |
9:45 | |
| | |
Example 2: Cube with Magnetic Field |
5:36 | |
| |
Faraday's Law |
70:38 |
| | |
Intro |
0:00 | |
| | |
Faraday's Law |
0:14 | |
| | |
| Coil Connected to Ammeter |
0:29 | |
| | |
| Introducing a Magnet |
1:08 | |
| | |
| Moving the Magnet Forward and Backward |
1:33 | |
| | |
| Flux Increasing in Time |
2:20 | |
| | |
| Induced Electro Motive Force EMF |
4:20 | |
| | |
| Iron Core Square with Battery and Switch, Ammeter |
5:22 | |
| | |
| Close the Switch, Current Appears |
6:11 | |
| | |
Lenz's Law |
9:17 | |
| | |
| Wire with Current I and Wire Loop |
9:30 | |
| | |
| Magnetic Field is Into the Page |
10:14 | |
| | |
| Current Induced in Wire to Oppose Change in Flux |
12:54 | |
| | |
| Example: Two Wires with Resistance and Uniform Magnetic Field |
16:00 | |
| | |
Increasing B |
29:02 | |
| | |
| Coil of 100 Turns |
29:20 | |
| | |
| B Perpendicular to Coil |
30:47 | |
| | |
| Flux Through Each Turn |
32:25 | |
| | |
Rotating Coil |
37:36 | |
| | |
| Consider a Big Magnet and Rectangular Coil with many Turns |
37:49 | |
| | |
| Rotating Coil With Angular Velocity 'w' |
41:49 | |
| | |
Example 1: Loop |
9:51 | |
| | |
Example 2: Solenoid |
6:57 | |
| | |
Example 3: Wrapped Square |
7:16 | |
| |
Motional EMF |
60:17 |
| | |
Intro |
0:00 | |
| | |
Moving a Conducting Rod in Magnetic Field |
0:24 | |
| | |
| Rod Moving in a Plane with Velocity 'v' |
0:49 | |
| | |
| Charges Piles Up and Down Until Electric Force Balance 'B' |
7:59 | |
| | |
| Equilibrium |
9:30 | |
| | |
| Potential Difference, Distance to Length of Wire |
9:59 | |
| | |
Rod Pulled By External Agent |
11:30 | |
| | |
| Resistance to Wire |
12:01 | |
| | |
| Introducing Uniform Magnetic Field into The page |
12:14 | |
| | |
| Finding Flux |
14:45 | |
| | |
| Power Delivered to Resistance |
17:01 | |
| | |
| Force Exerted by 'B' on Rod |
19:10 | |
| | |
| Power By Agent |
22:26 | |
| | |
Sliding Rod |
23:08 | |
| | |
| Resistance with a Sliding Rod and Magnetic Field 'B' |
23:35 | |
| | |
| Push With Initial Velocity 'V0' |
24:01 | |
| | |
| Finding Current = I |
25:20 | |
| | |
Rotating Rod |
36:10 | |
| | |
| Magnetic Field into The Page |
36:19 | |
| | |
| Rod fixed in Plane and Rotating |
36:40 | |
| | |
| Induced EMF in Segment |
40:00 | |
| | |
Example 1: Bar in Magnetic Field |
6:15 | |
| | |
Example 2: Rod in Magnetic Field |
11:08 | |
| |
Induced Electric Field |
65:19 |
| | |
Intro |
0:00 | |
| | |
Change B to Induce E |
0:54 | |
| | |
| Loop with Magnetic Field B |
1:10 | |
| | |
| Flux is Positive With Choice of 'n' |
2:45 | |
| | |
| Suppose Magnetic Field is Changing |
3:04 | |
| | |
| B Changing with time Flux (>0) |
3:24 | |
| | |
| Change in Electric Field Induces magnetic Field |
20:34 | |
| | |
Example |
21:08 | |
| | |
| Cylinder with Magnetic Field |
21:20 | |
| | |
| Fill With Radius 'r' |
22:11 | |
| | |
| Turn Off the Field |
22:30 | |
| | |
| Magnetic Flux Through Big Loop |
29:59 | |
| | |
AC Generator |
38:28 | |
| | |
| Magnetic Field with Coil of Many Turns |
38:50 | |
| | |
| As the Coil Rotates Flux is Induced |
39:18 | |
| | |
| Coil Rotated by Angle |
40:29 | |
| | |
| Coil Connected to The Ring and End Connected to Lamp |
42:12 | |
| | |
| Kinetic Energy Strike the Coil and Rotating Coil will Produce Electric Energy |
45:12 | |
| | |
Example 1: Electric Field |
12:09 | |
| | |
Example 2: Electric Field |
7:00 | |
| |
Inductance |
71:10 |
| | |
Intro |
0:00 | |
| | |
Mutual Inductance |
0:10 | |
| | |
| Two Coils |
0:35 | |
| | |
| Current is Time Dependent |
0:54 | |
| | |
| Flux Proportional |
1:55 | |
| | |
| Magnetic Flux in Coil 2 |
2:08 | |
| | |
| Induced EMF |
2:40 | |
| | |
| Flux Through 2nd Coil Proportional to Current in First Coil |
4:07 | |
| | |
| Mutual Inductance |
5:30 | |
| | |
| Suppose Current is in 2nd Coil |
9:28 | |
| | |
Example |
12:15 | |
| | |
| Two Coils M=0.001 |
12:26 | |
| | |
| Φ= Mi1 |
14:17 | |
| | |
| Induced EMF |
15:44 | |
| | |
Example |
18:30 | |
| | |
| Solenoid with N turns |
18:40 | |
| | |
| B inside Solenoid |
21:05 | |
| | |
| Φ Through the Ring |
22:14 | |
| | |
Self Inductance |
27:50 | |
| | |
| Single Coil with Current |
28:33 | |
| | |
| I with Time Dependent |
28:54 | |
| | |
| Φ Proportional to B , Proportional to I |
30:00 | |
| | |
| Induced EMF =-di/dt |
31:27 | |
| | |
Example 1: Circular Wire |
15:46 | |
| | |
Example 2: Two Coils |
9:54 | |
| | |
Example 3: Coil |
7:24 | |
| |
RL Circuits |
85:19 |
| | |
Intro |
0:00 | |
| | |
Current Raising |
0:45 | |
| | |
| Battery and Switch with Resistance and Inductance |
1:17 | |
| | |
| Close s1 at T=0 |
2:27 | |
| | |
| With out Inductor , Current is E/R |
4:03 | |
| | |
| I at T=0 |
9:51 | |
| | |
| Vb-Va= -Ir |
15:05 | |
| | |
| Log (i-e/r) |
19:51 | |
| | |
Current Declining |
27:16 | |
| | |
| Resistance R and Inductance |
27:37 | |
| | |
| I= E/R |
28:37 | |
| | |
| Switch is On at T=0 |
29:10 | |
| | |
Example |
39:46 | |
| | |
| Battery and Resistance R Connected with Inductor |
39:55 | |
| | |
| Time Constant l/R |
40:58 | |
| | |
| Time to Reach Half Time |
41:59 | |
| | |
| per τ (1-1/e) |
44:36 | |
| | |
Magnetic Energy |
45:47 | |
| | |
| E-IR-Ldi/dt |
46:26 | |
| | |
| Power Derived By Current |
46:51 | |
| | |
| Magnetic Energy Stored in Conductor |
52:48 | |
| | |
| U=Li2 |
55:28 | |
| | |
Magnetic Energy Density |
57:49 | |
| | |
| Solenoid |
58:18 | |
| | |
| U=1/2 Li2 |
59:03 | |
| | |
| Energy Density |
60:45 | |
| | |
Example 1: Circuit 1 |
6:13 | |
| | |
Example 2: Circuit 2 |
16:54 | |
| |
Circuit Oscillation |
82:26 |
| | |
Intro |
0:00 | |
| | |
Oscillation in LC Circuit: Qualitative Analysis |
0:30 | |
| | |
| Circuit with Capacitance and Inductance |
1:27 | |
| | |
Comparison with a Spring Block System |
4:57 | |
| | |
| Close the Switch, Let the Block Move |
5:51 | |
| | |
| At V=0 |
7:06 | |
| | |
LC Circuit Oscillation :Quantitative Analysis |
15:07 | |
| | |
| U Total = Ue + U m |
17:26 | |
| | |
Example RLC |
29:25 | |
| | |
| Battery =12V, Capacitor and Inductor |
29:54 | |
| | |
| Switch at B F> t |
31:42 | |
| | |
| Damped Oscillation |
50:14 | |
| | |
Example 1: LC Circuit 1 |
7:34 | |
| | |
Example 2: LC Circuit 2 |
16:19 | |
| | |
Example 3: RLC Circuit |
6:52 | |
| |
Maxwell's Equations |
72:35 |
| | |
Intro |
0:00 | |
| | |
Displacement Current |
1:29 | |
| | |
| Ampere's Law |
3:04 | |
| | |
| Surface Bounded by Path |
3:48 | |
| | |
| I Current Going Through Surface |
4:53 | |
| | |
| Charging a Capacitor |
9:55 | |
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Maxwell's Equation |
18:26 | |
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| Integral Form |
18:53 | |
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| E.da =Q/e0 in Closed Surface |
18:55 | |
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| Absence of Magnetic Monopoles |
19:55 | |
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| Flux Through the Surface Bounded By C |
22:26 | |
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| Ampere's Law |
23:01 | |
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Plane Electromagnetic Wave |
31:03 | |
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| Electric and Magnetic Field |
31:27 | |
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Example |
39:20 | |
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| Electromagnetic Wave Traveling in X Direction |
39:40 | |
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| Lamda=c/f |
41:30 | |
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| B=E/C |
43:49 | |
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Energy and Momentum Carried by EM Waves |
44:34 | |
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| Energy Density |
46:35 | |
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| Area in Y-Z Plane , Wave in X -Direction |
48:53 | |
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| Energy Crossing Per Unit Area |
52:53 | |
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| Pointing Vector |
53:11 | |
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| Reflection of Radioactive |
60:26 | |
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Example 1: Cylindrical Region |
8:36 | |
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Example 2: Electric Field of EM Wave |
3:16 | |