Chapter 22 – Gauss' Law and Flux
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Gauss's Law II
Gauss’s law II If a lightning bolt strikes a car (unless it is a convertible), electrons would quickly (in the order of nano seconds) move to the surface, so it is almost an ideal conductive shell that you can hide inside during a lightning storm! Reading: Mazur 24.7-25.2 Deriving Gauss’s law Applying Gauss’s law Electric potential energy Electrostatic work LECTURE 7 1 24.7 Deriving Gauss’s law Gauss’s law states that the flux through a closed surface is proportional to the enclosed charge, �"#$, such that �"#$ Φ& = �) LECTURE 7 2 Question: 24.7-1 (Flux from point charge) Consider a spherical Gaussian surface of radius � with a point charge � at the center. � 1 ⃗ The flux through a surface is given by Φ& = ∮1 � ⋅ ��. Using this definition for flux and Coulomb's law, calculate the flux through the Gaussian surface in terms of �, �, � and any constants. LECTURE 7 3 Question: 24.7-1 (Flux from point charge) answer Consider a spherical Gaussian surface of radius � with a point charge � at the center. � 1 ⃗ The flux through a surface is given by Φ& = ∮1 � ⋅ ��. Using this definition for flux and Coulomb's law, calculate the flux through the Gaussian surface in terms of �, �, � and any constants. The electric field is always normal to the Gaussian surface and has equal magnitude at all points on the surface. Therefore 1 1 1 � Φ = 3 � ⋅ ��⃗ = 3 ��� = � 3 �� = � 4��6 = � 4��6 = 4��� & �6 1 1 1 7 From Gauss’s law Φ& = 89 7 : Therefore Φ& = = 4���, and �) = 89 ;<= LECTURE 7 4 Reading quiz (Problem 24.70) There is a Gauss's law for gravity analogous to Gauss's law for electricity. -
Ancient Narrative Volume 1
History into fiction: the metamorphoses of the Mithras myths ROGER BECK Toronto Dedicated to Reinhold Merkelbach, whose explorations of ancient narra- tive and the mystery cults have always seemed to me profoundly well oriented, even when I would not follow the same path in detail. This article is neither about a particular ancient novel nor about the genre of the ancient novel in general. But it is about story-telling in the ancient world, and about the metamorphosis which stories undergo when they pass through the crucible of religious invention. Its subject, then, is narrative fiction — narrative fiction as the construction of sacred myth and of myth’s dramatic counterpart, ritual performance. The fictions I shall explore are the myths and rituals of the Mithras cult. Some of these fictions, I shall argue, are elaborations of events and fantasies of the Neronian age: on the one hand, events in both Italy and the orient cen- tred on the visit of Tiridates of Armenia to Rome in 66; on the other hand, the heliomania of the times, a solar enthusiasm focused on, and in some measure orchestrated by, the emperor himself. What I am not offering is an explanation of Mithraism and its origins. In the first place, our subject is story and the metamorphosis of story, not relig- ion. In the second place, I would not presume to ‘explain’ Mithraism, or any other religion for that matter, by Euhemeristic reduction to a set of historical or pseudo-historical antecedents. In speaking of the ‘invention’ of Mithraism and of its ‘fictions’, moreover, I intend no disrespect. -
Maxwell's Equations
Maxwell’s Equations Matt Hansen May 20, 2004 1 Contents 1 Introduction 3 2 The basics 3 2.1 Static charges . 3 2.2 Moving charges . 4 2.3 Magnetism . 4 2.4 Vector operations . 5 2.5 Calculus . 6 2.6 Flux . 6 3 History 7 4 Maxwell’s Equations 8 4.1 Maxwell’s Equations . 8 4.2 Gauss’ law for electricity . 8 4.3 Gauss’ law for magnetism . 10 4.4 Faraday’s law . 11 4.5 Ampere-Maxwell law . 13 5 Conclusion 14 2 1 Introduction If asked, most people outside a physics department would not be able to identify Maxwell’s equations, nor would they be able to state that they dealt with electricity and magnetism. However, Maxwell’s equations have many very important implications in the life of a modern person, so much so that people use devices that function off the principles in Maxwell’s equations every day without even knowing it. 2 The basics 2.1 Static charges In order to understand Maxwell’s equations, it is necessary to understand some basic things about electricity and magnetism first. Static electricity is easy to understand, in that it is just a charge which, as its name implies, does not move until it is given the chance to “escape” to the ground. Amounts of charge are measured in coulombs, abbreviated C. 1C is an extraordi- nary amount of charge, chosen rather arbitrarily to be the charge carried by 6.41418 · 1018 electrons. The symbol for charge in equations is q, sometimes with a subscript like q1 or qenc. -
Units in Electromagnetism (PDF)
Units in electromagnetism Almost all textbooks on electricity and magnetism (including Griffiths’s book) use the same set of units | the so-called rationalized or Giorgi units. These have the advantage of common use. On the other hand there are all sorts of \0"s and \µ0"s to memorize. Could anyone think of a system that doesn't have all this junk to memorize? Yes, Carl Friedrich Gauss could. This problem describes the Gaussian system of units. [In working this problem, keep in mind the distinction between \dimensions" (like length, time, and charge) and \units" (like meters, seconds, and coulombs).] a. In the Gaussian system, the measure of charge is q q~ = p : 4π0 Write down Coulomb's law in the Gaussian system. Show that in this system, the dimensions ofq ~ are [length]3=2[mass]1=2[time]−1: There is no need, in this system, for a unit of charge like the coulomb, which is independent of the units of mass, length, and time. b. The electric field in the Gaussian system is given by F~ E~~ = : q~ How is this measure of electric field (E~~) related to the standard (Giorgi) field (E~ )? What are the dimensions of E~~? c. The magnetic field in the Gaussian system is given by r4π B~~ = B~ : µ0 What are the dimensions of B~~ and how do they compare to the dimensions of E~~? d. In the Giorgi system, the Lorentz force law is F~ = q(E~ + ~v × B~ ): p What is the Lorentz force law expressed in the Gaussian system? Recall that c = 1= 0µ0. -
Examining the Transference Between Mithraism and Christianity Peter J
\ The Sword and the Cross: Examining the Transference between Mithraism and Christianity Peter J. Decker III Advisor: Dr. Elizabeth Manwell Ph. D .. Kalamazoo College Co-Chair of Classics Department I - A paper submitted in partial fulfillment of the requirements for the degr~e of Bachelor of ~rts at - - Kalamazoo College. 2013 Table of Contents Acknowledgments ......................... ~ .... : ......................................................ii I. The Cult ofMithras: Imagery, Practices, and Beliefs ............................... .1-21 II. Examining the Transference between Mithraism and Christianity ............... ~ .. 23-38 III. Appendix .......................· ............................................................. 39 Bibliography .................... ·................................................................. 40-44 / 11 Acknowledgements I am deeply grateful to my loving parents who made it possible to attend Kalamazoo College and allow me to further my studies in Classics. Without their financial and emotional support I would not have been able to complete this Senior Independent Project (SIP). Love you Mom and Dad! I am also deepl_y thankful to the Todd family and their generous grant, the Todd Memorial Classics Study Abroad Grant, which allowed me to travel to Italy and gain the inspiration for the topic of my SIP. I would like to express aspecial thanks to my SIP advisor Prof. Manwell, for putting up with all my procrastination and my challenging writing. I hope you didn't spend to many nights up late editing my drafts. Without all of you none of this would have been possible. Thank you very much. 1 I. The Cult ofMithras: Imagery, Practices, and Beliefs In the spring of 2011 an American atheist group put up a billboard in downtown New York City which read: "Born of a virgin on December 25th, known to his 12 disciples as "the Son of God, and resurrected three days after his death, we wish a Happy Birthday to Mithras, the mythical Persian god imagined over 600 years before that other guy .. -
6.007 Lecture 5: Electrostatics (Gauss's Law and Boundary
Electrostatics (Free Space With Charges & Conductors) Reading - Shen and Kong – Ch. 9 Outline Maxwell’s Equations (In Free Space) Gauss’ Law & Faraday’s Law Applications of Gauss’ Law Electrostatic Boundary Conditions Electrostatic Energy Storage 1 Maxwell’s Equations (in Free Space with Electric Charges present) DIFFERENTIAL FORM INTEGRAL FORM E-Gauss: Faraday: H-Gauss: Ampere: Static arise when , and Maxwell’s Equations split into decoupled electrostatic and magnetostatic eqns. Electro-quasistatic and magneto-quasitatic systems arise when one (but not both) time derivative becomes important. Note that the Differential and Integral forms of Maxwell’s Equations are related through ’ ’ Stoke s Theorem and2 Gauss Theorem Charges and Currents Charge conservation and KCL for ideal nodes There can be a nonzero charge density in the absence of a current density . There can be a nonzero current density in the absence of a charge density . 3 Gauss’ Law Flux of through closed surface S = net charge inside V 4 Point Charge Example Apply Gauss’ Law in integral form making use of symmetry to find • Assume that the image charge is uniformly distributed at . Why is this important ? • Symmetry 5 Gauss’ Law Tells Us … … the electric charge can reside only on the surface of the conductor. [If charge was present inside a conductor, we can draw a Gaussian surface around that charge and the electric field in vicinity of that charge would be non-zero ! A non-zero field implies current flow through the conductor, which will transport the charge to the surface.] … there is no charge at all on the inner surface of a hollow conductor. -
Symmetry • the Concept of Flux • Calculating Electric Flux • Gauss's
Topics: • Symmetry • The Concept of Flux • Calculating Electric Flux • Gauss’s Law • Using Gauss’s Law • Conductors in Electrostatic Equilibrium PHYS 1022: Chap. 28, Pg 2 1 New Topic PHYS 1022: Chap. 28, Pg 3 For uniform field, if E and A are perpendicular, define If E and A are NOT perpendicular, define scalar product General (surface integral) Unit of electric flux: N . m2 / C Electric flux is proportional to the number of field lines passing through the area. And to the total change enclosed PHYS 1022: Chap. 28, Pg 4 2 + + PHYS 1022: Chap. 28, Pg 5 + + PHYS 1022: Chap. 28, Pg 6 3 r + ½r + 2r PHYS 1022: Chap. 28, Pg 7 r + ½r + 2r PHYS 1022: Chap. 28, Pg 8 4 A metal block carries a net positive charge and put in an electric field. 1) 0 What is the electric field inside? 2) positive 3) Negative 4) Cannot be determined If there is an electric field inside the conductor, it will move the charges in the conductor to where each charge is in equilibrium. That is, net force = 0 therefore net field = 0! PHYS 1022: Chap. 28, Pg 9 A metal block carries a net charge and 1) All inside the conductor put in an electric field. Where does 2) All on the surface the net charge reside ? 3) Some inside the conductor, some on the surface The net field = 0 inside, and so the net flux through any surface drawn inside the conductor = 0. Therefore the net charge inside = 0! PHYS 1022: Chap. 28, Pg 10 5 PHYS 1022: Chap. -
Connects Charge and Field 3. Applications of Gauss's
Gauss Law 1. Review on 1) Coulomb’s Law (charge and force) 2) Electric Field (field and force) 2. Gauss’s Law: connects charge and field 3. Applications of Gauss’s Law Coulomb’s Law and Electric Field l Coulomb’s Law: the force between two point charges Coulomb’s Law and Electric Field l Coulomb’s Law: the force between two point charges ! q q F = K 1 2 rˆ e e r2 12 Coulomb’s Law and Electric Field l Coulomb’s Law: the force between two point charges ! q q F = K 1 2 rˆ e e r2 12 l The electric field is defined as Coulomb’s Law and Electric Field l Coulomb’s Law: the force between two point charges ! q q F = K 1 2 rˆ e e r2 12 l The electric field is defined! as ! F E ≡ q0 and is represented through field lines. Coulomb’s Law and Electric Field l Coulomb’s Law: the force between two point charges ! q q F = K 1 2 rˆ e e r2 12 l The electric field is defined! as ! F E ≡ q0 and is represented through field lines. l The force a charge experiences in an electric filed is Coulomb’s Law and Electric Field l Coulomb’s Law: the force between two point charges ! q q F = K 1 2 rˆ e e r2 12 l The electric field is defined! as ! F E ≡ q0 and is represented through field lines. l The force a charge experiences in an electric filed is ! ! F = q0E Coulomb’s Law and Electric Field l Coulomb’s Law: the force between two point charges ! q q F = K 1 2 rˆ e e r2 12 l The electric field is defined! as ! F E ≡ q0 and is represented through field lines. -
21. Maxwell's Equations. Electromagnetic Waves
University of Rhode Island DigitalCommons@URI PHY 204: Elementary Physics II -- Slides PHY 204: Elementary Physics II (2021) 2020 21. Maxwell's equations. Electromagnetic waves Gerhard Müller University of Rhode Island, [email protected] Robert Coyne University of Rhode Island, [email protected] Follow this and additional works at: https://digitalcommons.uri.edu/phy204-slides Recommended Citation Müller, Gerhard and Coyne, Robert, "21. Maxwell's equations. Electromagnetic waves" (2020). PHY 204: Elementary Physics II -- Slides. Paper 46. https://digitalcommons.uri.edu/phy204-slides/46https://digitalcommons.uri.edu/phy204-slides/46 This Course Material is brought to you for free and open access by the PHY 204: Elementary Physics II (2021) at DigitalCommons@URI. It has been accepted for inclusion in PHY 204: Elementary Physics II -- Slides by an authorized administrator of DigitalCommons@URI. For more information, please contact [email protected]. Dynamics of Particles and Fields Dynamics of Charged Particle: • Newton’s equation of motion: ~F = m~a. • Lorentz force: ~F = q(~E +~v ×~B). Dynamics of Electric and Magnetic Fields: I q • Gauss’ law for electric field: ~E · d~A = . e0 I • Gauss’ law for magnetic field: ~B · d~A = 0. I dF Z • Faraday’s law: ~E · d~` = − B , where F = ~B · d~A. dt B I dF Z • Ampere’s` law: ~B · d~` = m I + m e E , where F = ~E · d~A. 0 0 0 dt E Maxwell’s equations: 4 relations between fields (~E,~B) and sources (q, I). tsl314 Gauss’s Law for Electric Field The net electric flux FE through any closed surface is equal to the net charge Qin inside divided by the permittivity constant e0: I ~ ~ Qin Qin −12 2 −1 −2 E · dA = 4pkQin = i.e. -
A) Electric Flux B) Field Lines Gauss'
Electricity & Magnetism Lecture 3 Today’s Concepts: A) Electric Flux Gauss’ Law B) Field Lines Electricity & Magnetism Lecture 3, Slide 1 Your Comments “Is Eo (epsilon knot) a fixed number? ” “epsilon 0 seems to be a derived quantity. Where does it come from?” q 1 q ˆ ˆ E = k 2 r E = 2 2 r IT’S JUST A r 4e or r CONSTANT 1 k = 9 x 109 N m2 / C2 k e = 8.85 x 10-12 C2 / N·m2 4e o o “I fluxing love physics!” “My only point of confusion is this: if we can represent any flux through any surface as the total charge divided by a constant, why do we even bother with the integral definition? is that for non-closed surfaces or something? These concepts are a lot harder to grasp than mechanics. WHEW.....this stuff was quite abstract.....it always seems as though I feel like I understand the material after watching the prelecture, but then get many of the clicker questions wrong in lecture...any idea why or advice?? Thanks 05 Electricity & Magnetism Lecture 3, Slide 2 Electric Field Lines Direction & Density of Lines represent Direction & Magnitude of E Point Charge: Direction is radial Density 1/R2 07 Electricity & Magnetism Lecture 3, Slide 3 Electric Field Lines Legend 1 line = 3 mC Dipole Charge Distribution: “Please discuss further how the number of field lines is determined. Is this just convention? I feel Direction & Density as if the "number" of field lines is arbitrary, much more interesting. because the field is a vector field and is defined for all points in space. -
Chapter 5 Capacitance and Dielectrics
Chapter 5 Capacitance and Dielectrics 5.1 Introduction...........................................................................................................5-3 5.2 Calculation of Capacitance ...................................................................................5-4 Example 5.1: Parallel-Plate Capacitor ....................................................................5-4 Interactive Simulation 5.1: Parallel-Plate Capacitor ...........................................5-6 Example 5.2: Cylindrical Capacitor........................................................................5-6 Example 5.3: Spherical Capacitor...........................................................................5-8 5.3 Capacitors in Electric Circuits ..............................................................................5-9 5.3.1 Parallel Connection......................................................................................5-10 5.3.2 Series Connection ........................................................................................5-11 Example 5.4: Equivalent Capacitance ..................................................................5-12 5.4 Storing Energy in a Capacitor.............................................................................5-13 5.4.1 Energy Density of the Electric Field............................................................5-14 Interactive Simulation 5.2: Charge Placed between Capacitor Plates..............5-14 Example 5.5: Electric Energy Density of Dry Air................................................5-15 -
Power-Invariant Magnetic System Modeling
POWER-INVARIANT MAGNETIC SYSTEM MODELING A Dissertation by GUADALUPE GISELLE GONZALEZ DOMINGUEZ Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY August 2011 Major Subject: Electrical Engineering Power-Invariant Magnetic System Modeling Copyright 2011 Guadalupe Giselle González Domínguez POWER-INVARIANT MAGNETIC SYSTEM MODELING A Dissertation by GUADALUPE GISELLE GONZALEZ DOMINGUEZ Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Approved by: Chair of Committee, Mehrdad Ehsani Committee Members, Karen Butler-Purry Shankar Bhattacharyya Reza Langari Head of Department, Costas Georghiades August 2011 Major Subject: Electrical Engineering iii ABSTRACT Power-Invariant Magnetic System Modeling. (August 2011) Guadalupe Giselle González Domínguez, B.S., Universidad Tecnológica de Panamá Chair of Advisory Committee: Dr. Mehrdad Ehsani In all energy systems, the parameters necessary to calculate power are the same in functionality: an effort or force needed to create a movement in an object and a flow or rate at which the object moves. Therefore, the power equation can generalized as a function of these two parameters: effort and flow, P = effort × flow. Analyzing various power transfer media this is true for at least three regimes: electrical, mechanical and hydraulic but not for magnetic. This implies that the conventional magnetic system model (the reluctance model) requires modifications in order to be consistent with other energy system models. Even further, performing a comprehensive comparison among the systems, each system’s model includes an effort quantity, a flow quantity and three passive elements used to establish the amount of energy that is stored or dissipated as heat.