| Week | Date | Lectures/Exams | Readings | Topics | 
 
  | 1 | Tu  | Lecture 1:
  Introduction Slides ACTs
 | None | Introduction | 
 
  | Th  | Lecture 2:
  Coulomb's Law Slides ACTs
 | Ch 22.1-4 | 
   Electrostatic
       Phenomena (rubber rods & glass rods)  How do we Interpret the results??
 Torsion balance gives spatial dependence
 
   Superposition of
       Forces Force Comparison:
       Electrical vs Gravitational The Electric Field  | 
 
  | 2 | Tu  | Lecture 3:
  Electric Fields Slides ACTs
 | Ch 22.4-22.7,
  23.1  | 
   Define Electric
       Field in terms of force on "test charge"Lines of ForceExample
       Calculations: Discrete: Electric Dipole
 Continuous: Infinite Line of Charge
 | 
 
  | Th  | Lecture 4:
  Gauss's Law Slides ACTs
 | Ch 23   | 
   Gauss' Law:
       Motivation & DefinitionCoulomb's Law as a
       consequence of Gauss' LawCharges on
       Conductors:  Where are they?
 
   Applications of
       Gauss' Law  Infinite Line of Charge
 Infinite Sheet of Charge
 Two infinite sheets of charge
 Shortcuts
 Uniform Charged Sphere
 | 
 
  | 3 | Tu  | Lecture 5:
  Electric Potential Slides ACTs
 | Ch 24.1-4 | 
   Introduce Concept
       of Electric Potential Is it well-defined? i.e. is Electric Potential a property of the space as is
  the Electric Field?
 
   Define
       EquipotentialsExamples Charged Spherical Shell
 N point charges
 Electric Dipole
 
   Can we determine
       the Electric Field if we know the Electric Potential?  | 
 
  | Th  | Lecture 6:
  Electric Potential Slides ACTs
 | Ch 24, 25.1 | 
   Brief Review of
       Potential from last lectureCalculate Electric
       Field of Dipole from PotentialEquipotentials and
       ConductorsElectric Potential
       Energy of Charge in External Electric Field
 stored in the Electric Field itself (next time)
 | 
 
  | 4 | Tu  | Lecture 7:
  Capacitance Slides ACTs
 | Ch 25.1-5 | 
   Energy stored in
       the Electric Field as distinguished from electric potential energy of a charge located in an
  electric field.
 
   Definition of
       CapacitanceExample
       Calculations Parallel Plate Capacitor
 Cylindrical Capacitor
 
   Combinations of Capacitors Capacitors in Parallel
 Capacitors in Series
 | 
 
  | Th  | Lecture 8:
  Capacitance Slides ACTs
 | Ch 25 | 
   Calculate Energy
       Stored in CapacitorCalculate Energy
       Density in Electric FieldDefine Dielectric
       ConstantModify Gauss’ Law
       to include Dielectrics  | 
 
  | 5 | Tu  | Lecture 9:
  Review Slides
 | Ch 22-25 | Coulomb's Law or Gauss' Law
 Law of Superposition
 Electric Field, Potential Function, Electric Potential Energy, Field Lines,
  Equipotentials
 Conductors and Insulators
 Capacitance, Dielectric constant
 E = -gradV, Capacitors: parallel, series, energy
 | 
 
  | Th  | Lecture 10:
  Simple Circuits Slides ACTs
 | Ch 26,27.1 (rest of Ch 27 optional)
 | Capacitors
 Batteries
 Resistors
 
   Resistors in
       Series & ParallelKirchoff's Rules Loop Rule (V is independent of path)
 Junction Rule (Charge is conserved)
 | 
 
  | 6 | Tu  | Lecture 11: RC
  Circuits Slides ACTs
 | Ch 26.6 (rest of Ch 27 optional)
 | 
   Power &
       (non-ideal) Batteries (from last time)Calculate Charging
       of capacitor through a ResistorCalculate
       Discharging of capacitor through a Resistor  | 
 
  | Th  | Lecture 12:
  Magnetic Force Slides ACTs
 | Ch 28.1, 2 | 
   Introduction to
       Magnetic Phenomena Bar magnets & Magnetic Field Lines
 Source of Fields: Monopoles? Currents?
 
   Diversion:
       Relativity and E & M Special Relativity Þ Magnetic forces MUST exist!!
 
   Magnetic forces:
       The Lorentz Force equationMotion of charged
       particle in a Constant Magnetic Field.  | 
 
  | 7 | Tu  | Lecture 13:
  Forces & Magnetic Dipoles Slides ACTs
 | Ch 28 | 
   Application of
       equation for trajectory of charged particle in a constant magnetic
       field: the Cyclotron.Magnetic Force on
       a current-carrying wireCurrent Loops Magnetic Dipole Moment
 Torque (when in constant B field)
 Potential Energy (when in constant B field)
 | 
 
  | Th  | Lecture 14: The
  Laws of Biot-Savart & Ampere Slides ACTs
 | Ch 29.1-4 | 
   Fundamental Law
       for Calculating Magnetic Field Biot-Savart Law (brute force)
 Ampere’s Law (high symmetry)
 
   Example: Calculate
       Magnetic Field of Infinite Straight Wire from Biot-Savart Law
 from Ampere’s Law
 
   Calculate Force on
       Two Parallel Current-Carrying Conductors  | 
 
  | 8 | Tu  | Lecture 15:
  Magnetic Fields Slides ACTs
 | Ch 29.1-4 | 
   Calculate Magnetic
       Fields Inside a Long Straight Wire
 Infinite Current Sheet
 Solenoid
 Toroid
 Circular Loop
 | 
 
  | Th  | Lecture 16:
  Faraday's Law Slides ACTs
 | Ch 30.1-5 | 
   Induction EffectsFaraday’s Law
       (Lenz’ Law) Energy Conservation with induced currents?
 
   Faraday’s Law in
       terms of Electric Fields Betatron
 | 
 
  | 10 | Tu  | Lecture 17:
  Review Slides
 | Ch 26-30 | Biot-Savart Law, Ampere's Law, Faraday’s Law
 Magnetic Field, Resistance, Magnetic Moment, Potential Energy, Magnetic Flux
 Kirchoff's Laws, Resistors: parallel,series, resistivity, Power in circuits,
  Force on currents, Torque on current loops.
 | 
 
  | Th  | Lecture 18:
  Self-Inductance Slides ACTs
 | Ch 30 | 
   Concept of
       Self-InductanceDefinition of
       Self-InductanceCalculation of
       Self-Inductance for Simple CasesRL CircuitsEnergy in
       Magnetic FieldMutual Inductance  | 
 
  | 11 | Tu  | Lecture 19:
  Oscillations: LC Circuits Slides ACTs
 | Ch 31.3 | 
   Qualitative
       descriptions: LC circuits (ideal inductor)
 LC circuits (L with finite R)
 
   Quantitative
       descriptions: LC circuits (ideal inductor)
 ---Frequency of oscillations
 ---Energy conservation?
 
   LC circuits (L
       with finite R) Frequency of oscillations
 Damping factor
 | 
 
  | Th  | Lecture 20: AC
  Circuits Slides ACTs
 | Ch 31.1-5 | Can a circuit be built with real components (ie resistance) which sustains
  the oscillations we saw in an LC circuit?
 Phases for driven circuits with R, C, and L
 Defined as a rotating vector
 Phase difference between current & voltage for Resistors, Capacitors, and
  Inductors.
 
   Application to
       Driven Series LCR Circuit: General solution
 | 
 
  | 13 | Tu  | Lecture 21: AC
  Circuits Slides ACTs
 | Ch 31.6-7 | 
   Driven Series LCR
       Circuit: General solution
 Resonance condition
 ..Resonant frequency
 ..Sharpness of resonance = Q
 Power considerations
 ..Power factor depends on impedance
 Voltage changes
 Faraday’s Law in action gives induced primary current.
 Power considerations
 | 
 
  | Th  | Lecture 22:
  Electromagnetic Waves Slides ACTs
 | Ch 32, 33.4 | 
   Electromagnetic
       Waves: ExperimentalAmpere’s Law Is
       Incomplete: Displacement CurrentReview of Wave
       Properties (remember the 111 finale?)Electromagnetic
       Waves: Theory Maxwell’s Equations contain the wave equation!
 The velocity of electromagnetic waves = c
 The relationship between E and B in an e-m wave
 Energy in e-m waves: the Poynting vector
 | 
 
  | 13 | Tu  | Lecture 23:
  Polarization Slides ACTs
 | Ch 33.7 | 
   Linearly
       Polarized e-m WavesLinear Polarizers
       (Law of Malus)Circular
       Polarization Quarter-Wave Plates
 | 
 
  | Th  | Lecture 24:
  Reflection & Refraction Slides ACTs
 | Ch 33.6 | 
   Polarization
       recapOverview : waves
       in materials & geometric opticsReflectionIndex of
       RefractionSnell’s Law for
       RefractionIntensity of
       reflected, refracted waves Total Internal Reflection
 Reflection: Brewster’s Angle
 Scattering
 | 
 
  | 14 | Tu  | Lecture 25:
  Review Slides
 | Ch 30-33 | Ampere’s Law (revisited)
 Inductance, Phasors, Resonance, Reactances, Impedance, Displacement Current,
  Poynting Vector, Polarization
   States.
 RL Circuit behavior, Energy in inductor, LC Oscillations, LCR series circuit
  solution, Average Power in AC circuits, E-M Wave Eqn, Speed of E-M waves, LP
  Transmission, Reflection & Refraction.
 | 
 
  | Th  | Lecture 26:
  Mirrors & Lenses Slides
 | Ch 34.1-3 | 
   Overview :
       Nothing new here!Concave Spherical
       Mirrors The Mirror Eqn, Magnification, Sign Conventions
 
   Planar &
       Convex Spherical MirrorsLenses The Lens Equation
 | 
 
  | 15 | Tu  | Lecture 27:
  Optical Instruments Slides ACTs
 | Ch 34.4 | 
   The Lensmaker’s
       FormulaMultiple LensesThe Eye Corrective Lenses for Myopic & Hypertropic Eyes
 
   Magnifiers &
       MicroscopesTelescopes  | 
 
  | Th  | Lecture 28: All
  Act Review Slides
 | See Lecture Slides |  | 
 
  | 16 | Tu  | Lecture 29: The
  Last Waltz Slides
 | Ch 22-34 | Coulomb's Law or Gauss' Law
 Law of Superposition
 Biot-Savart Law, Ampere's Law
 Faraday's Law (Lenz's Law)
 Electric Field, Potential Difference, Electric Potential Energy, Field Lines,
  Equipotentials, Conductors and Insulators, Capacitance, Dielectric constant
 Magnetic Field, Resistance, Magnetic Moment, Potential Energy, Magnetic Flux,
  Inductance, Phasors, Resonance, Reactances
 Displacement Current, Poynting Vector, Polarization States
 E = -gradV , Capacitors: parallel, series, energy
 Kirchoff's Laws, Resistors: parallel,series, resistivity, Power in circuits,
  Force on currents, Torque on current loops
 RL Circuit behavior, Energy in inductor, LC Oscillations, LCR series circuit
  solution, Average Power in AC circuits
 Mirror/Lens Equation
 | 
 
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