• 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
Magnetic Fields and Forces
Magnetic Fields and Forces

Powerpoint
Powerpoint

Possible new effects in superconductive tunnelling
Possible new effects in superconductive tunnelling

... a r e constant. A difficulty, due to the fact that we have a system containing two disjoint superconducting r e gions, a r i s e s if we t r y to describe q u a s i - p a r t i c l e s by the usual t~goliubov operators 2). This i s because states defined as eigeafanetions of the Bogotinbev q u a s i ...
43.1 Vector Fields and their properties
43.1 Vector Fields and their properties

... Figure 161. Gravitation force field Some of the geometric concepts, like curves are also described by vector fields, as we shall see later. The notion of limit for a vector-field can be defined in a manner similar to that of functions of several variables. 43.1.4 Definition: be a vector field, wher ...
Which statement best explains why it is possible to define an
Which statement best explains why it is possible to define an

Electroweak Unification as Classical Field Theory
Electroweak Unification as Classical Field Theory

P2420100
P2420100

Since we will be studying electromagnetic waves, let`s review some
Since we will be studying electromagnetic waves, let`s review some

... A radio wave can be detected with a receiving antenna wire that is parallel to the electric field: è E generates an oscillating current along the antenna wire. ...
Magnetism
Magnetism

... The flux only depends on the portion of the magnetic field that is perpendicular to the area in which is passes through. So when the magnetic field direction is not perpendicular to the area the equation for flux becomes Φ = B A cos θ The SI unit of magnetic flux is the Weber (W) ...
Discussion 3
Discussion 3

P132 Chapter 31
P132 Chapter 31

Astrophysics by Jonathan Chan
Astrophysics by Jonathan Chan

...  High voltage applied across the electrodes  Cathode rays (streams of electrons) flow from the cathode towards the anode. (–ve to +ve) Manipulation of cathode rays: Structures built into or around cathode ray tube, manipulating the rays:  Further electrodes built into cathode ray tube creating an ...
ELECTROMAGNETISM: (Boctor, Ch. 9, p. 332)
ELECTROMAGNETISM: (Boctor, Ch. 9, p. 332)

Angular momenta dynamics in magnetic and electric
Angular momenta dynamics in magnetic and electric

... Usually when describing angular momentum in atomic or molecular physics, we use a quantummechanical approach. However, there are problems, mostly connected with the description of states with large angular-momentum quantum numbers (M  43 = = = 433,, say, in molecular physics, where the classical ap ...
PHY_211_ADDITIONAL_REVISION_QUESTION_
PHY_211_ADDITIONAL_REVISION_QUESTION_

Magnetic quenching of time-reversed light in photorefractive diluted magnetic semiconductors
Magnetic quenching of time-reversed light in photorefractive diluted magnetic semiconductors

Electromagnetism - Lecture 9 Dielectric Materials
Electromagnetism - Lecture 9 Dielectric Materials

Devil physics The baddest class on campus IB Physics Physics I
Devil physics The baddest class on campus IB Physics Physics I

Magnetism - Ms. Gamm
Magnetism - Ms. Gamm

Introduction to the Fractional Quantum Hall Effect
Introduction to the Fractional Quantum Hall Effect

Fractional Charge
Fractional Charge

QUANTUM ELECTRODYNAMICS AND GRAVITATION
QUANTUM ELECTRODYNAMICS AND GRAVITATION

The Can Crusher
The Can Crusher

Lecture_10
Lecture_10

Powerpointreviewchap16
Powerpointreviewchap16

... N. If this charge is removed and a 6 C charge is placed at that point instead, what force will it feel? ...
< 1 ... 391 392 393 394 395 396 397 398 399 ... 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