The fields and self-force of a constantly accelerating spherical shell by Andrew M. Steane Proceedings A Volume 470(2162):20130480 February 8, 2014 ©2014.

Slides:



Advertisements
Similar presentations
Which is the correct expression for work
Advertisements

Unit 1 Day 16: Electric Potential due to any Charge Distribution
The electric flux may not be uniform throughout a particular region of space. We can determine the total electric flux by examining a portion of the electric.
Applications of Gauss’s Law
Chapter 22--Examples.
Chapter 22: The Electric Field II: Continuous Charge Distributions
Electric Potential AP Physics Montwood High School R. Casao.
VEKTORANALYS Kursvecka 6 övningar. PROBLEM 1 SOLUTION A dipole is formed by two point sources with charge +c and -c Calculate the flux of the dipole.
Gauss’s law and its applications
A note on ‘Einstein's special relativity beyond the speed of light by James M. Hill and Barry J. Cox’ by Hajnal Andréka, Judit X. Madarász, István Németi,
Multiple steadily translating bubbles in a Hele-Shaw channel by Christopher C. Green, and Giovani L. Vasconcelos Proceedings A Volume 470(2163):
Example: An insulating solid sphere of radius R has a uniform positive volume charge density and total charge Q. a)Find the electric potential at a point.
Graphing motion. Displacement vs. time Displacement (m) time(s) Describe the motion of the object represented by this graph This object is at rest 2m.
Locomotion pattern generation and mechanisms of a new biped walking machine by Hun-ok Lim, Y Ogura, and Atsuo Takanishi Proceedings A Volume 464(2089):
Relative to the effort it would take to thoroughly read the chapter once, how much effort did you put into doing the reading assignment? a) 0-20% b) 20-50%
Extinction rate, historical population structure and ecological role of the Caribbean monk seal by Loren McClenachan, and Andrew B Cooper Proceedings B.
Asymptotic analysis of double-carrier, space-charge- limited transport in organic light-emitting diodes by Sarah E. Feicht, Ory Schnitzer, and Aditya S.
Wednesday, February 4, 2015MAT 146. Wednesday, February 4, 2015MAT 146.
A Charged, Thin Sheet of Insulating Material
Homework 1-4 Find all the force vectors and then add the vectors to find the total force.
A Charged, Thin Sheet of Insulating Material
Chapter 24 Gauss’s Law.
Example: Potential Difference of Point Charges Consider a point charge q. What is the potential difference between point x 1 and point x 2 ? q x2x2 x1x1.
Problem #34 (a) Example 23.8 (a) Consider a uniformly charged thin-walled right circular cylindrical shell having total charge Q, radius R, and height.
Average 68.4 Median Highest 100 Lowest 26 Section Section Section Section
Calculate Electric Potential: Example A conducting sphere of radius R 1 =0.5m is placed at the center of a conducting spherical shell of inner and outer.
Slide 1 Electric Field Lines 10/29/08. Slide 2Fig 25-21, p.778 Field lines at a conductor.
Exam Average 78.4 Median 84 Outline Applications of Gauss’s Law - The single Fixed Charge -Field of a sphere of charge -Field of a.
Nadiah Alanazi Gauss’s Law 24.3 Application of Gauss’s Law to Various Charge Distributions.
Antennas Hertzian Dipole –Current Density –Vector Magnetic Potential –Electric and Magnetic Fields –Antenna Characteristics.
Gravity and Orbits The gravitational force between two objects:
Charles Allison © 2000 Chapter 22 Gauss’s Law HW# 5 : Chap.22: Pb.1, Pb.6, Pb.24, Pb.27, Pb.35, Pb.46 Due Friday: Friday, Feb 27.
Gauss’ Law.
Numerical study of shearing of a microfibre during friction testing of a microfibre array by Ajeet Kumar, and Chung-Yuen Hui Proceedings A Volume 467(2129):
Electricity and Magnetism Review 1: Units 1-6
Electric Flux and Gauss Law
Gauss’sLaw 1 P05 - The first Maxwell Equation A very useful computational technique This is important!
1 Gauss’s Law For r > a Reading: Chapter Gauss’s Law Chapter 28.
A thin-shelled reptile from the Late Triassic of North America and the origin of the turtle shell by Walter G Joyce, Spencer G Lucas, Torsten M Scheyer,
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Cylinder loading in transient motion representing flow under a wave group by T. Stallard, P.H. Taylor, C.H.K. Williamson, and A.G.L. Borthwick Proceedings.
Reception and learning of electric fields in bees by Uwe Greggers, Gesche Koch, Viola Schmidt, Aron Dürr, Amalia Floriou-Servou, David Piepenbrock, Martin.
CHAPTER 24 : GAUSS’S LAW 24.1) ELECTRIC FLUX
The role of particle shape on the stress distribution in a sandpile by I Zuriguel, and T Mullin Proceedings A Volume 464(2089): January 8, 2008 ©2008.
When ecosystem services interact: crop pollination benefits depend on the level of pest control by Ola Lundin, Henrik G. Smith, Maj Rundlöf, and Riccardo.
Application of Gauss’ Law to calculate Electric field:
Copyright © 2009 Pearson Education, Inc. Chapter 22 Gauss’s Law.
Modelling of elastic properties of sintered porous materials by A. V. Manoylov, F. M. Borodich, and H. P. Evans Proceedings A Volume 469(2154):
Chapter 23 Electric Potential. Basics The potential due to an electric dipole is just the sum of the potentials due to each charge, and can be calculated.
Chapter 23 Electric Potential.
-Electric Potential due to Continuous Charge Distributions AP Physics C Mrs. Coyle.
Q22.1 A spherical Gaussian surface (#1) encloses and is centered on a point charge +q. A second spherical Gaussian surface (#2) of the same size also encloses.
Tue. Feb. 3 – Physics Lecture #26 Gauss’s Law II: Gauss’s Law, Symmetry, and Conductors 1. Electric Field Vectors and Electric Field Lines 2. Electric.
Electricity and Magnetism Review 2: Units 7-11 Mechanics Review 2, Slide 1.
2.1 Position, Velocity, and Speed 2.1 Displacement  x  x f - x i 2.2 Average velocity 2.3 Average speed  
Example 5.1 Worked on the Board!
Gauss’s Law (III) Examples.
Tue. Jan. 27 – Physics Lecture #23 Electric Field, Continued (and Continuous!) 1. Electric Field due to Continuous Charge Distributions Warm-up: Consider.
Unit 1 Day 11: Applications of Gauss’s Law Spherical Conducting Shell A Long Uniform Line of Charge An Infinitely Large, Thin Plane of Charge Experimental.
Electric Potential The scalar function V determines the vector field E! The reference point O is arbitrary, where V(O)=0. It is usually put at infinity.
Chapter 11 - Gravity. Example 3 The International Space Station Travels in a roughly circular orbit around the earth. If it’s altitude is 385 km above.
Charles Allison © 2000 Chapter 22 Gauss’s Law.. Charles Allison © 2000 Problem 57.
Electric Fields Due to Continuous Charge Distributions
Copyright © 2009 Pearson Education, Inc. Applications of Gauss’s Law.
Electric Potential (III)
Hertzian Dipole Current Density Vector Magnetic Potential
-Calculation of Moments of Inertia for Rigid Objects of Different Geometries -Parallel Axis Theorem AP Physics C Mrs. Coyle.
PHY 2049: Physics II Tutoring Center is open in room NPB 1100, M-F 10:00AM -3:00PM. It is free. Hopefully all webassign problems have been solved. Please.
Exam 2 review.
23 Electric Potential all sections
Presentation transcript:

The fields and self-force of a constantly accelerating spherical shell by Andrew M. Steane Proceedings A Volume 470(2162): February 8, 2014 ©2014 by The Royal Society

Electric field lines in the xy-plane, in the instantaneous rest frame, for a spherical charged shell of radius R=1/2 undergoing rigid hyperbolic motion along the x-axis with proper acceleration a0=1/L0=1. Andrew M. Steane Proc. R. Soc. A 2014;470: ©2014 by The Royal Society

Electric field E (thick line) and potential ϕ (thin line) on the x-axis for a sphere of radius R=1/2 with unit charge accelerating in the x-direction with proper acceleration a0=1/L0=1. Andrew M. Steane Proc. R. Soc. A 2014;470: ©2014 by The Royal Society

(a) Self-force as a function of R, for L0=1, as calculated by numerical integration (points) and by equation (5.11) (solid line). Andrew M. Steane Proc. R. Soc. A 2014;470: ©2014 by The Royal Society