6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Derivatives and Electrostatics Corinne Manogue Tevian Dray

Slides:



Advertisements
Similar presentations
The divergence of E If the charge fills a volume, with charge per unit volume . R Where d is an element of volume. For a volume charge:
Advertisements

Gauss’s law Can we find a simplified way to perform electric-field calculations Yes, we take advantage of a fundamental relationship between electric charge.
Two questions: (1) How to find the force, F on the electric charge, Q excreted by the field E and/or B? (2) How fields E and/or B can be created?
Electric Flux Density, Gauss’s Law, and Divergence
17 mayo 2011V CONGRESO NACIONAL DE ENSENANZA DE LA FISICA ENSEÑANDO A LOS ESTUDIANTES A PENSAR COMO FÍSICOS Tevian Dray & Corinne Manogue
ENTC 3331 RF Fundamentals Dr. Hugh Blanton ENTC 3331.
ELECTROSTATICS-1 ONLINE TEST Q.NO.ANSWER Q.NO.ANSWER Q.NO.ANSWER
EE2030: Electromagnetics (I)
Nadiah Alanazi 1 Chapter 24 Gauss’s Law 24.1 Electric Flux 24.2 Gauss’s Law 24.3 Application of Gauss’s Law to Various Charge Distributions 24.4 Conductors.
Fundamentals of Applied Electromagnetics
19-1 Physics I Class 19 The Electric Field What Is a Field?
Ch3 Quiz 1 First name ______________________ Last name ___________________ Section number ______ There is an electric field given by where E 0 is a constant.
2-7 Divergence of a Vector Field
Lecture 19 Exam II Average: Lecture 19 Today Brief review of Electrostatics (I) 1.Maxwell equations 2.Charge and current distributions.
20-1 Physics I Class 20 The Electric Field What Is a Field?
Average 68.4 Median Highest 100 Lowest 26 Section Section Section Section
2D case: If or then 2 or 3D cases: Several dimensions: U(x,y,z) Compact notation using vector del, or nabla: Another notation: Partial derivative is.
3. Differential operators
Hw: All Chapter 4 problems and exercises Chapter 5: Pr. 1-4; Ex. 1,2 Reading: Chapter 4.
Hw: All Chapter 4 problems and exercises Chapter 5: Pr. 1-4; Ex. 1,2 Reading: Chapter 4.
Vectors Sections 6.6. Objectives Rewrite a vector in rectangular coordinates (in terms of i and j) given the initial and terminal points of the vector.
Outline Area vector Vector flux More problems Solid angle Proof of Gauss’s Law.
PHY 042: Electricity and Magnetism
Lecture 13 Basic Laws of Vector Algebra Scalars: e.g. 2 gallons, $1,000, 35ºC Vectors: e.g. velocity: 35mph heading south 3N force toward center.
Copyright © Cengage Learning. All rights reserved. 16 Vector Calculus.
Operators. 2 The Curl Operator This operator acts on a vector field to produce another vector field. Let be a vector field. Then the expression for the.
Notes 13 ECE 2317 Applied Electricity and Magnetism Prof. D. Wilton
Dr. Hugh Blanton ENTC Gauss’s Law Dr. Blanton - ENTC Gauss’s Theorem 3 Recall Divergence literally means to get farther apart from a line.
ENE 325 Electromagnetic Fields and Waves Lecture 3 Gauss’s law and applications, Divergence, and Point Form of Gauss’s law 1.
Applied Electricity and Magnetism
5 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Vectors and Transformations Corinne Manogue Tevian Dray
4 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Active-Engagment Strategies that help students learn how to 'Think Like a Physicist' Corinne Manogue.
EMLAB 1 Chapter 3. Gauss’ law, Divergence. EMLAB 2 Displacement flux : Faraday’s Experiment charged sphere (+Q) insulator metal Two concentric.
Chapter 27. A uniformly charged rod has a finite length L. The rod is symmetric under rotations about the axis and under reflection in any plane containing.
7 October 2010http:// Vector Integrals and Electrostatics Corinne Manogue Tevian Dray
President UniversityErwin SitompulEEM 4/1 Dr.-Ing. Erwin Sitompul President University Lecture 4 Engineering Electromagnetics
Poisson’s Equation Section 5.2 (“Fish’s” Equation!) Comparison of properties of gravitational fields with similar properties of electrostatic fields (Maxwell’s.
Tue. Feb. 3 – Physics Lecture #25 Gauss’s Law I: Field Lines and Flux 1. Electric Field Vectors and Electric Field Lines 2. Electric Field and Electric.
Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0, the other
1 Engineering Electromagnetics Essentials Chapter 1 Vector calculus expressions for gradient, divergence, and curl Introduction Chapter 2 and.
8.022 (E&M) – Lecture 3 Topics:  Electric potential
Electrostatics Chapter Properties of Physical Objects Mass/Inertial: – Gravity mass: inertia in gravitational interaction – Kinetic mass: inertia.
Divergence Theorem and E-field1 The Divergence Theorem and Electrical Fields © Frits F.M. de Mul.
Gauss’ Law Chapter 23. Electric field vectors and field lines pierce an imaginary, spherical Gaussian surface that encloses a particle with charge +Q.
Problem 3 p. 45 Electric potential on ring’s axis From Chapter 2:
Warm UP.  What are projection vectors?  MM4A10. Students will understand and use vectors. a. Represent vectors algebraically and geometrically. b.
CALCULUS III CHAPTER 5: Orthogonal curvilinear coordinates
Last Time Faraday's Law Inductance and RL (RLC) circuit.
Flux and Gauss’s Law Spring Last Time: Definition – Sort of – Electric Field Lines DIPOLE FIELD LINK CHARGE.
LINE,SURFACE & VOLUME CHARGES
Applied Electricity and Magnetism
Geometry-Part 8.
Chapter 3 Overview.
Chapter 3. Gauss’ law, Divergence
Chapter 9 Vector Calculus.
Electricity and Magnetism
Electromagnetics II.
1.4 Curvilinear Coordinates Cylindrical coordinates:
Fields and Waves I Lecture 8 K. A. Connor Y. Maréchal
Gauss’s Law.
Electricity and Magnetism
Lecture 19 Maxwell equations E: electric field intensity
Electrostatic Boundary Value Problems Ref: Elements of Electromagnetics by Matthew N. O. Sadiku.
Question for the day Can the magnitude of the electric charge be calculated from the strength of the electric field it creates?
Task 1 Knowing the components of vector A calculate rotA and divA.
Copyright © Cengage Learning. All rights reserved.
Task 1 Knowing the components of vector A calculate rotA and divA.
Physics I Class 19 The Electric Field.
Fundamentals of Applied Electromagnetics
DEPARTMENT OF PHYSICS GOVT.PG COLLEGE RAJOURI
Presentation transcript:

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Derivatives and Electrostatics Corinne Manogue Tevian Dray

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Scalar Fields

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Scalar Fields in 3-D

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Vector Fields We use the idea of field lines for electric fields because: –They are a concrete representation of Gauss’s law—they only end on charges. It is difficult to see three dimensional vectors on a two dimensional graph.

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA The Concept of Flux

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Visualizing Flux Initially, define the location of the point charge to be at the origin of a rectangular coordinate system: > Point:=[0,0,0]; > a:=Point[1];b:=Point[2];c:=Point[3]; Find the electric field of the point charge: > r:=sqrt((x-a)^2+(y-b)^2+(z-c)^2); > Efield:=(q/(4*Pi*epsilon))*grad(-1/r,[x,y,z]);

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Flux Maple Worksheet

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Relating Multiple Representations

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Flux out of the Top and Bottom of a Cube

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Flux out of an Entire Cube The total flux out of the cube is equal to the divergence of the field times the volume of the cube.

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Visualizing Divergence

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA The Divergence Theorem Divide your volume into many small boxes. Use the definition of divergence on each one.

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Differential Form of Gauss’s Law

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Curvilinear Coordinates

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Curvilinear Basis Vectors

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Curvilinear Basis Vectors

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA The Vector Differential

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA The Vector Differential

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA The Geometry of Change

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA The Master Formula where

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA The Hill

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Visualization—Gradient

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Cross Product

6 October 2010XIII SEMANA DE LA ENSENANZA DE LA FISICA Cross Product