PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 3:

Slides:



Advertisements
Similar presentations
Chapter 6 Electrostatic Boundary-Value Problems
Advertisements

Lecture 19 Exam II Average: Lecture 19 Today Brief review of Electrostatics (I) 1.Maxwell equations 2.Charge and current distributions.
Chapter 7 – Poisson’s and Laplace Equations
Lecture 12: 2nd-order Vector Operators Lecture 11 meaningless Laplace’s Equation is one of the most important in physics.
Chapter 4: Solutions of Electrostatic Problems
EEE340Lecture 161 Solution 3: (to Example 3-23) Apply Where lower case w is the energy density.
EM & Vector calculus #3 Physical Systems, Tuesday 30 Jan 2007, EJZ Vector Calculus 1.3: Integral Calculus Line, surface, volume integrals Fundamental theorems.
02/03/2014PHY 712 Spring Lecture 81 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 8: Start reading Chapter 4 Multipole moment.
3/30/2015PHY 752 Spring Lecture 261 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 107 Plan for Lecture 26:  Chap. 19 in Marder  Properties.
02/17/2014PHY 712 Spring Lecture 141 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 14: Start reading Chapter 6 1.Maxwell’s.
02/16/2015PHY 712 Spring Lecture 141 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 14: Start reading Chapter 6 1.Maxwell’s full.
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.
01/31/2014PHY 712 Spring Lecture 71 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 7: Start reading Chapter 3 Solution of Poisson.
1/21/2015PHY 712 Spring Lecture 31 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 3: Reading: Chapter 1 in JDJ 1.Review of electrostatics.
EMLAB 1 6. Capacitance. EMLAB 2 Contents 1.Capacitance 2.Capacitance of a two-wire line 3.Poisson’s and Laplace’s equations 4.Examples of Laplace’s equation.
1 EEE 431 Computational Methods in Electrodynamics Lecture 3 By Dr. Rasime Uyguroglu.
02/05/2014PHY 712 Spring Lecture 91 PHY 712 Electrodynamics 11-11:50 AM MWF Olin 107 Plan for Lecture 9: Continue reading Chapter 4 Dipolar fields.
Chapter 4: Solutions of Electrostatic Problems 4-1 Introduction 4-2 Poisson’s and Laplace’s Equations 4-3 Uniqueness of Electrostatic Solutions 4-4 Methods.
Chapter 4 : Solution of Electrostatic ProblemsLecture 8-1 Static Electromagnetics, 2007 SpringProf. Chang-Wook Baek Chapter 4. Solution of Electrostatic.
11/30/2015PHY 711 Fall Lecture 371 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 37 Review of.
1/24/2014PHY 712 Spring Lecture 61 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 6: Continue reading Chapter 2 1.Methods of.
1 LAPLACE’S EQUATION, POISSON’S EQUATION AND UNIQUENESS THEOREM CHAPTER LAPLACE’S AND POISSON’S EQUATIONS 6.2 UNIQUENESS THEOREM 6.3 SOLUTION OF.
Finding electrostatic potential Griffiths Ch.3: Special Techniques week 3 fall EM lecture, 14.Oct.2002, Zita, TESC Review electrostatics: E, V, boundary.
EXAMPLES OF SOLUTION OF LAPLACE’s EQUATION NAME: Akshay kiran E.NO.: SUBJECT: EEM GUIDED BY: PROF. SHAILESH SIR.
1 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 29: Start reading Chap. 15 – Radiation from collisions of charged particles 1.Overview.
EEE 431 Computational Methods in Electrodynamics
PHY 711 Classical Mechanics and Mathematical Methods
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 6:
Christopher Crawford PHY
Representation Theory
PHY 711 Classical Mechanics and Mathematical Methods
Introduction to groups having infinite dimension
Uniqueness Theorem vanishes on S vanishes in V
PHY 712 Electrodynamics 11-11:50 AM MWF Olin 107 Plan for Lecture 14:
Christopher Crawford PHY
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 1:
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 9:
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 12:
PHY 711 Classical Mechanics and Mathematical Methods
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 9:
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 3:
PHY 752 Solid State Physics
Maxwell’s full equations; effects of time varying fields and sources
PHY 752 Solid State Physics Plan for Lecture 30: Chap. 13 of GGGPP
PHY 711 Classical Mechanics and Mathematical Methods
PHY 711 Classical Mechanics and Mathematical Methods
Finish reading Chapter 6
PHY 711 Classical Mechanics and Mathematical Methods
PHY 711 Classical Mechanics and Mathematical Methods
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 11:
PHY 752 Solid State Physics Inhomogeneous semiconductors
Electromagnetic waves due to specific sources
Reading: Chapter in JDJ
Reading: Chapters #5 in Shankar; quantum mechanical systems in 1-dim
PHY 711 Classical Mechanics and Mathematical Methods
PHY 711 Classical Mechanics and Mathematical Methods
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 6:
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 8:
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 1:
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 7:
PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 22:
Read Chapter # 9 in Shankar Commutator formalism and
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 10:
Review Chapter 1-8 in Jackson
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 11:
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 2:
Maxwell’s full equations; effects of time varying fields and sources
Finish reading Chapter 6
Presentation transcript:

PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 3: Reading: Chapter 1 in JDJ Review of electrostatics with one-dimensional examples Poisson and Laplace Equations Green’s Theorem and their use in electrostatics 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

1/18/2019 PHY 712 Spring 2019 -- Lecture 3

Poisson and Laplace Equations We are concerned with finding solutions to the Poisson equation: and the Laplace equation: The Laplace equation is the “homogeneous” version of the Poisson equation. The Green's theorem allows us to determine the electrostatic potential from volume and surface integrals: 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

Poisson equation -- continued 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

General comments on Green’s theorem This general form can be used in 1, 2, or 3 dimensions. In general, the Green's function must be constructed to satisfy the appropriate (Dirichlet or Neumann) boundary conditions. Alternatively or in addition, boundary conditions can be adjusted using the fact that for any solution to the Poisson equation, other solutions may be generated by use of solutions of the Laplace equation 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

“Derivation” of Green’s Theorem 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

“Derivation” of Green’s Theorem 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

1/18/2019 PHY 712 Spring 2019 -- Lecture 3

1/18/2019 PHY 712 Spring 2019 -- Lecture 3

1/18/2019 PHY 712 Spring 2019 -- Lecture 3

Comment about the example and solution This particular example is one that is used to model semiconductor junctions where the charge density is controlled by introducing charged impurities near the junction. The solution of the Poisson equation for this case can be determined by piecewise solution within each of the four regions. Alternatively, from Green's theorem in one-dimension, one can use the Green's function 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

Notes on the one-dimensional Green’s function 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

Construction of a Green’s function in one dimension 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

Summary 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

One dimensional Green’s function in practice This expression gives the same result as previously obtained for the example r(x) and more generally is appropriate for any neutral charge distribution. 1/18/2019 PHY 712 Spring 2019 -- Lecture 3

1/18/2019 PHY 712 Spring 2019 -- Lecture 3

1/18/2019 PHY 712 Spring 2019 -- Lecture 3

1/18/2019 PHY 712 Spring 2019 -- Lecture 3

1/18/2019 PHY 712 Spring 2019 -- Lecture 3