• 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
Chapter 31
Chapter 31

PHYS 112
PHYS 112

Science - BC Curriculum - Province of British Columbia
Science - BC Curriculum - Province of British Columbia

... • law of conservation of energy applications: — gravitational potential energy ...
26 Magnetism
26 Magnetism

Quantum Mechanics
Quantum Mechanics

The Orbital magnetic moment in terms of Bohr magneton in
The Orbital magnetic moment in terms of Bohr magneton in

CBSE-SAMPLE PAPER 3 -2011 -Class XII- Subject
CBSE-SAMPLE PAPER 3 -2011 -Class XII- Subject

... i) an isolated positive point charge (q>o) ii) an isolated negative point charge (q>o) 2. Two electric lines of force do not interact. Explain why? 3. Define the term electric dipole moment. 4. Give two properties of electric lines of force. Sketch them for a positively charged metallic sphere. 5. D ...
Document
Document

PowerPoint
PowerPoint

Maxwell*s Equation*s in integral form
Maxwell*s Equation*s in integral form

... An induction coil is connected to a transmitter The transmitter consists of two spherical electrodes separated by a narrow gap The discharge between the electrodes exhibits an oscillatory behavior at a very high frequency Sparks were induced across the gap of the receiving electrodes when the freque ...
effect of an uniform electric field on charge transfer processes. a
effect of an uniform electric field on charge transfer processes. a

... bonds will break and new bonds will be formed. The proton or methyl transfer, respectively, will thus be produced. An interesting conclusion of this work is that the mere presence of an external electric field may produce an acceleration in the reaction rate without the presence of any catalyst. Cle ...
File
File

... There are two sets of “hand” rules that can be used to determine the direction of the magnetic field around an electrical conductor Your choice of which set of rules to use depends on which system you use to describe electric current: ...
The Standard Model (SM) describes the fundamental particles of the
The Standard Model (SM) describes the fundamental particles of the

Charged Particles
Charged Particles

Metals I: Free Electron Model
Metals I: Free Electron Model

Giant microwave tunability in FeGaB/lead magnesium niobate-lead titanate multiferroic composites J. Lou,
Giant microwave tunability in FeGaB/lead magnesium niobate-lead titanate multiferroic composites J. Lou,

PDF of Solution of assignment 8
PDF of Solution of assignment 8

H3- PHYS102 - Honors Lab-3H
H3- PHYS102 - Honors Lab-3H

Paper
Paper

... Systems of spherical molecules, such as the rare gases, have been intensively studied over a broad range of temperatures and densities using pair interactions of Lennard-Jones (LJ) type. Extensive calculations of the equation of state of the LJ fluid have been performed with Monte Carlo (MC) and mol ...
Student Exploration Sheet: Growing Plants
Student Exploration Sheet: Growing Plants

Lecture 2 Quantum mechanics in one dimension
Lecture 2 Quantum mechanics in one dimension

Kelly Nguyen Electrical Energy And Capacitors Definitions
Kelly Nguyen Electrical Energy And Capacitors Definitions

Homework #8: Magnetic Force and Biot-Savart Law
Homework #8: Magnetic Force and Biot-Savart Law

... 1. [10 points] Suppose that an electron is released from rest in a region where there is a uniform electric field in the z-direction and a magnetic field in the x-direction. Determine the trajectory of the electron if it starts at the origin with velocity. ...
Recent Development in Density Functional Theory in the
Recent Development in Density Functional Theory in the

zeeman effect
zeeman effect

< 1 ... 463 464 465 466 467 468 469 470 471 ... 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