Electricity and Magnetism: Electrostatics

• L01v01: What is Charge
• L1v2: Electric Force
• L1v3: Rewrite the Unit Vector in Coulomb's Law
• L1v5: Analogy of Coulomb's Law and Gravity
• L2v1: Vector Fields
• L2v2: Kinds of Vector Fields
• L2v3: Electric Field of a Positive Point Charge
• L2v4: Superposition
• L2v5: Worked Example - Total Electric Field Due to 2 Charges
• L02v06: Electric Field Lines
• L3v1: Introduction to Electric Dipoles
• L3v2: Electric Dipole Moment of 2 Charges
• L3v3: Definition of the Dipole Moment
• L3v4: Worked Example - Dipole Moment of 3 Charges
• L3v5: Dipole Moment is Independent of Origin
• L3v7: Dipole in a Non-uniform Field Demo
• L3DDv1: Electric Field of a Dipole Everywhere in Space
• L3DDv2: Rewrite the Electric Field of a Dipole
• L3DDv3: Electric Field Far Away from the Dipole
• L3DDv4: Rewrite Dipole Far Field with p and theta
• L3DDv5: Final Form of the Dipole Far FIeld
• L4v1: Electric Field of a Continuous Charge Source
• L4v2: Electric Field from a Rod on the Symmetry Axis Using Angles and Symmetry
• L4v3: Continuous Charge Distribution Electric Field Calculation with Source to Point Vector
• L4v4: Electric Field from a Rod on the Symmetry Axis Using the Source to Point Vector