Christopher Crawford PHY

Slides:



Advertisements
Similar presentations
Electromagnetism week 9 Physical Systems, Tuesday 6.Mar. 2007, EJZ Waves and wave equations Electromagnetism & Maxwell’s eqns Derive EM wave equation and.
Advertisements

1 Electromagnetism We want to apply the reaction theory developed in the first few lectures to electronuclear interactions. It is worthwhile reviewing.
8/5/08Lecture 2 Part 21 Maxwell’s Equations of the Electromagnetic Field Theory Gauss’s Law – charge makes an electric field The magnetic field is solenoidal.
Electromagnetism Giancoli Ch Physics of Astronomy, winter week 7
02/19/2014PHY 712 Spring Lecture 151 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 15: Finish reading Chapter 6 1.Some details.
02/18/2015PHY 712 Spring Lecture 151 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 15: Finish reading Chapter 6 1.Some details.
Lecture 4: Boundary Value Problems
Chapter 7 Electrodynamics
Electromagnetic radiation l MAXWELL'S EQUATIONS: are four differential equations summarizing nature of electricity and magnetism: (formulated by James.
Magnetostatic Fields Electrostatic field : stuck charge distribution
EEE 431 Computational methods in Electrodynamics Lecture 1 By Rasime Uyguroglu.
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Classical electrodynamics.
Chapter 5 Magnetostatics 5.1 The Lorentz Force Law 5.2 The Biot-Savart Law 5.3 The Divergence and Curl of 5.4 Magnetic Vector Potential.
Maxwell’s Equations If we combine all the laws we know about electromagnetism, then we obtain Maxwell’s equations. These four equations plus a force law.
Electromagnetism I Week 8. Contents Overview Overview Coulomb’s Law Coulomb’s Law Current Current Voltage Voltage Resistance Resistance Energy and Power.
Lecture 23 Static field Dynamic Field Lecture 23 Faraday’s Law.
PHY 417G: Review Christopher Crawford
Maxwell’s Equations and Electromagnetic Waves
PHY 520 Introduction Christopher Crawford
Finish EM Ch. 5: Magnetostatics Methods of Math
Introduction to materials physics #2 Week 2: Electric and magnetic interaction and electromagnetic wave 1.
Electromagnetism INEL 4152 CH 9 Sandra Cruz-Pol, Ph. D. ECE UPRM Mayag ü ez, PR.
Christopher Crawford PHY 417G: Introduction Christopher Crawford
Waves from the Sun Electromagnetic Wave Electric field – The electric field E at a point is defined as the force per unit charge experienced by a small.
Finish EM Ch.5: Magnetostatics Methods of Math. Physics, Thus. 10 March 2011, E.J. Zita Lorentz Force Ampere’s Law Maxwell’s equations (d/dt=0) Preview:
Maxwell’s Equations are Lorentz Invariant
ELEN 340 Electromagnetics II Lecture 2: Introduction to Electromagnetic Fields; Maxwell’s Equations; Electromagnetic Fields in Materials; Phasor Concepts;
Maxwell’s Equations. Four equations, known as Maxwell’s equations, are regarded as the basis of all electrical and magnetic phenomena. These equations.
ELEC 401 MICROWAVE ELECTRONICS Lecture 1
Electromagnetic Theory
Forces on Fields Charles T. Sebens University of California, San Diego
Maxwell’s Equations in Terms of Potentials
Department of Electronics
Comparison of Magnetostatics and Electrostatics
Christopher Crawford PHY
§7.2 Maxwell Equations the wave equation
Time-dependent fields
Maxwell’s Equations.
Christopher Crawford PHY
Christopher Crawford PHY
Transverse Electromagnetic Waves in Free Space
Electromagnetics II.
ELEC 401 MICROWAVE ELECTRONICS Lecture 1
Christopher Crawford PHY 416G: Introduction Christopher Crawford
Christopher Crawford PHY
Christopher Crawford PHY
Christopher Crawford PHY
Chapter 5 Magnetostatics
Lecture 19 Maxwell equations E: electric field intensity
§5.2: Formulations of Magnetostatics
Christopher Crawford PHY
PHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101
Christopher Crawford PHY
§2.4 Conductors – capacitance
§7.2 Maxwell Equations the wave equation
The Maxwell equations.
Christopher Crawford PHY
Christopher Crawford PHY
Christopher Crawford PHY
Introduction: A review on static electric and magnetic fields
Maxwell’s Equations and Electromagnetic Waves
Basic Electromagnetics
Christopher Crawford PHY 311: Introduction Christopher Crawford
Maxwell’s Equations and Electromagnetic Waves
E&M I Griffiths Chapter 7.
Finish reading Chapter 6
This presentation uses a free template provided by FPPT.com Transformations of the electric and magnet field Rida khan.
Electromagnetism in Curved Spacetime
Finish reading Chapter 6
§7.2 Maxwell Equations the wave equation
Presentation transcript:

Christopher Crawford PHY 417 2014-02-27 §7.2 Maxwell Equations Christopher Crawford PHY 417 2014-02-27

Outline Review – TWO separate derivative chains (in space only) ES and MS formulations: potentials and Poisson’s equation THREE observations: a) Coulomb, b) Ampere, c) Faraday the third ties the derivative chains of the other two together TWO+1 cracks in the foundation – patching up space and time Scalar potential, Maxwell’s displacement current Example: potential momentum associated with a B-field Example: the displacement current through a capacitor Materials: THREE+1 charges and SIX currents Maxwell Equations – unified symmetry in space and time Differential & integral fields, potentials, boundary cond’s Space-time symmetry – ONE complete derivative chain Duality rotations – magnetic monopoles revisited

Two separate formulations ELECTROSTATICS Coulomb’s law MAGNETOSTATICS Ampère’s law

Two separate formulations ELECTROSTATICS MAGNETOSTATICS Faraday’s law stitches the two formulations together in space and time

One unified formulation ELECTROMAGNETISM Faraday’s law stitches the two formulations together in space and time Previous hint: continuity equation

TWO cracks in the foundation Faraday’s law appears to violate conservation of energy? Unified gauge transformation for V and A Continuity equation vs. Ampère’s law

Example: current through a capacitor Which surface should one use for Ampère’s law? Maxwell’s displacement current Fluid mechanical model Elasticity of medium –> EM waves On Faraday's Lines of Force (1855) On Physical Lines of Force (1961) The Dynamical Theory of the Electromagnetic Field (1865)

Example 7.8: potential momentum Charges moving in magnetic field Charges in abruptly changing magnetic field Magnetic field energy acts as “electromagnetic inertia”

Maxwell’s equations Integral & differential Potentials & wave eq. Boundary conditions Constitution equations Continuity equation Lorentz Force Field energy

Electrical properties of materials Same old THREE charges (plus one magnetic) Now: SIX currents, including displacement!

Unification of E and B Projections of electromagnetic field in space and time That is the reason for the twisted symmetry in field equations

Unification of D and H Summary

Duality Rotation (ε,1/μ) tensor behaves like i : converts between flux and flow Compare (E,B) to (x,y) in the complex plane

Conservation of Energy Similar to other fluxes x flows