• Study Resource
  • Explore Categories
    • Arts & Humanities
    • Business
    • Engineering & Technology
    • Foreign Language
    • History
    • Math
    • Science
    • Social Science

    Top subcategories

    • Advanced Math
    • Algebra
    • Basic Math
    • Calculus
    • Geometry
    • Linear Algebra
    • Pre-Algebra
    • Pre-Calculus
    • Statistics And Probability
    • Trigonometry
    • other →

    Top subcategories

    • Astronomy
    • Astrophysics
    • Biology
    • Chemistry
    • Earth Science
    • Environmental Science
    • Health Science
    • Physics
    • other →

    Top subcategories

    • Anthropology
    • Law
    • Political Science
    • Psychology
    • Sociology
    • other →

    Top subcategories

    • Accounting
    • Economics
    • Finance
    • Management
    • other →

    Top subcategories

    • Aerospace Engineering
    • Bioengineering
    • Chemical Engineering
    • Civil Engineering
    • Computer Science
    • Electrical Engineering
    • Industrial Engineering
    • Mechanical Engineering
    • Web Design
    • other →

    Top subcategories

    • Architecture
    • Communications
    • English
    • Gender Studies
    • Music
    • Performing Arts
    • Philosophy
    • Religious Studies
    • Writing
    • other →

    Top subcategories

    • Ancient History
    • European History
    • US History
    • World History
    • other →

    Top subcategories

    • Croatian
    • Czech
    • Finnish
    • Greek
    • Hindi
    • Japanese
    • Korean
    • Persian
    • Swedish
    • Turkish
    • other →
 
Profile Documents Logout
Upload
Free Fall of Elementary Particles
Free Fall of Elementary Particles

Electromagnetism G. L. Pollack and D. R. Stump The Exercise
Electromagnetism G. L. Pollack and D. R. Stump The Exercise

Physics 9 Fall 2010 - faculty.ucmerced.edu
Physics 9 Fall 2010 - faculty.ucmerced.edu

Practice exam 1
Practice exam 1

Lecture 09 - Purdue Physics
Lecture 09 - Purdue Physics

Document
Document

... physical models presented in the lectures. You are also expected to master the problemsolving techniques in the discussion sections and the homework. The exam will consist of 4 problems (each worth 20% of the total) and a set of multiple-choice questions (also worth 20% of the total). To receive a f ...
any
any

view pdf - Sub-Structure of the Electron
view pdf - Sub-Structure of the Electron

Magnetic Fields and Forces
Magnetic Fields and Forces

Bound magnetic polarons in semimagnetic quantum wells
Bound magnetic polarons in semimagnetic quantum wells

Millikan`s Experiment and Motion of Charges Lesson
Millikan`s Experiment and Motion of Charges Lesson

Chapter 7
Chapter 7

... Can not explain the line spectra for other elements due to electron-electron interactions.  Thus, the formula for Hydrogen can only be applied for that atom.  LEP #4. ...
Chapter 34
Chapter 34

202b399
202b399

Handout: Particle motion - Harvard
Handout: Particle motion - Harvard

First lecture, 7.10.03
First lecture, 7.10.03

... If you measure momentum P... you don’t know anything about X. If you measure position X... you don’t know anything about P. But in real life, don’t I know something about each? Don’t I also know that if a car left this morning and is already in Budapest, it’s going faster than if it’s still on Währi ...
ELECTRODYNAMICS—lecture notes second semester 2004 Ora Entin-Wohlman
ELECTRODYNAMICS—lecture notes second semester 2004 Ora Entin-Wohlman

... discontinuity in the normal component of the electric field. The tangential components are continuous. Exercise: The electric field of a uniformly charged (infinite) plane, of charge σ per unit area. By symmetry, (for a plane perpendicular to the z-axis), ...
Chapter30 - Academic Program Pages
Chapter30 - Academic Program Pages

... ξ = 2πfNabB sin(2πft) = ξ0 sin(2πft). This is the principle of the commercial alternating-current generator. (b) What value of Nab gives an emf with ξ0 = 150 V when the loop is rotated at 60.0 rev/s in a uniform magnetic field of 0.500T? 11. (a) It should be emphasized that the result, given in term ...
Student Text, pp. 504-505
Student Text, pp. 504-505

Unveiling the quantum critical point of an Ising chain
Unveiling the quantum critical point of an Ising chain

problem #3: measuring the magnetic field of permanent magents
problem #3: measuring the magnetic field of permanent magents

CH17 notes
CH17 notes

... Infinitely far away from all charged particles, V = 0. We commonly define the potential at a specific location V (r) as the potential difference between r and the point at infinity: V (r) = V (r) − V (∞) = V (r) − 0. ...
EXPERIMENT 11 Determination of e/m for the Electron Introduction
EXPERIMENT 11 Determination of e/m for the Electron Introduction

electric potential ( symbol V )
electric potential ( symbol V )

Slide 1
Slide 1

... In symbols: v || B  min. V (=0) ...
< 1 ... 497 498 499 500 501 502 503 504 505 ... 661 >

Aharonov–Bohm effect

The Aharonov–Bohm effect, sometimes called the Ehrenberg–Siday–Aharonov–Bohm effect, is a quantum mechanical phenomenon in which an electrically charged particle is affected by an electromagnetic field (E, B), despite being confined to a region in which both the magnetic field B and electric field E are zero. The underlying mechanism is the coupling of the electromagnetic potential with the complex phase of a charged particle's wavefunction, and the Aharonov–Bohm effect is accordingly illustrated by interference experiments.The most commonly described case, sometimes called the Aharonov–Bohm solenoid effect, takes place when the wave function of a charged particle passing around a long solenoid experiences a phase shift as a result of the enclosed magnetic field, despite the magnetic field being negligible in the region through which the particle passes and the particle's wavefunction being negligible inside the solenoid. This phase shift has been observed experimentally. There are also magnetic Aharonov–Bohm effects on bound energies and scattering cross sections, but these cases have not been experimentally tested. An electric Aharonov–Bohm phenomenon was also predicted, in which a charged particle is affected by regions with different electrical potentials but zero electric field, but this has no experimental confirmation yet. A separate ""molecular"" Aharonov–Bohm effect was proposed for nuclear motion in multiply connected regions, but this has been argued to be a different kind of geometric phase as it is ""neither nonlocal nor topological"", depending only on local quantities along the nuclear path.Werner Ehrenberg and Raymond E. Siday first predicted the effect in 1949, and similar effects were later published by Yakir Aharonov and David Bohm in 1959. After publication of the 1959 paper, Bohm was informed of Ehrenberg and Siday's work, which was acknowledged and credited in Bohm and Aharonov's subsequent 1961 paper.Subsequently, the effect was confirmed experimentally by several authors; a general review can be found in Peshkin and Tonomura (1989).
  • studyres.com © 2026
  • DMCA
  • Privacy
  • Terms
  • Report