• 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
Lab instruction Lab Semiconductor physics Course Modern Physics
Lab instruction Lab Semiconductor physics Course Modern Physics

... e) Switch on the current supply for the magnet and adjust the current to set a magnetic field of 1000 Gauss(0.1T) at the position where the sample is placed. The current supplied should be around 2A. f) Take out the sample holder from the Dewar. Place it between the poles of the electromagnets. The ...
if on the Internet, Press  on your browser to
if on the Internet, Press on your browser to

Word document
Word document

The Use and Abuse of “photon” in Nanomechanics – pdf
The Use and Abuse of “photon” in Nanomechanics – pdf

... same sort of skepticism prevailed during the development of those theories). In fact, this appears in both classical and quantum theories of electrodynamics, and plays a significant role in both. To review briefly, this is the effect of the field created by charge upon that very charge. One of two e ...
Atomic 1
Atomic 1

... In 1925 S. Goudsmit and G. Uhlenbeck, proposed that the electron must have an intrinsic (built in) angular momentum. This proposal runs into problems if it is considered classically, so we must regard this additional angular momentum an a purely quantum mechanical effect To explain the experimental ...
2 + - dubai
2 + - dubai

Electric field of a spherical shell Q
Electric field of a spherical shell Q

... "For my own part I wish the Bald Eagle had not been chosen the Representative of our Country. He is a Bird of bad moral Character. He does not get his Living honestly. You may have seen him perched on some dead Tree near the River, where, too lazy to fish for himself, he watches the Labour of the F ...
Quantum electrodynamic Aharonov
Quantum electrodynamic Aharonov

The Spectator-Induced Electromagnetic Effect on Meson Production
The Spectator-Induced Electromagnetic Effect on Meson Production

1 Electrostatics Lecture No : 14 Tittle : Faraday`s Law of Induction
1 Electrostatics Lecture No : 14 Tittle : Faraday`s Law of Induction

Accelerators - UC Davis Physics
Accelerators - UC Davis Physics

PSI AP 2 EMF Worksheet
PSI AP 2 EMF Worksheet

... 46. Which of the following will generate a current in a conducting loop? Select two answers: A. A bar magnet moving towards the loop. B. A bar magnet remaining stationary within the loop. C. The loop rotating on an axis perpendicular to the bar magnet. D. A magnet and the loop moving to the right w ...


... We know that when a sphere is placed in an electric field it acquires a dipole moment, and we expect that this dipole moment is proportional to the electric field. Let us denote the proportionality constant by α ( α is called the atomic polarizability). Namely, ...
File - SPHS Devil Physics
File - SPHS Devil Physics

... energy of the emitted electrons  The electron energy depends on the frequency of the incident light, and there is a certain minimum frequency below which no electrons are emitted.  Electrons are emitted with no time delay, i.e. no “build-up” of energy ...
No Slide Title
No Slide Title

11-10
11-10

10. Magnetism
10. Magnetism

The Stern Gerlach Experiment Abstract
The Stern Gerlach Experiment Abstract

... and r and ω are the radius and angular velocity of the motion. If this atom is placed inside a magnetic field, strongly varying in magnitude along the z-axis, the atom will experience a force Fz = −∇(−µ · B) = µz ∂Bz /∂z, which can range continuously over all values such that |Fz | ≤ |µ|∂Bz /∂z. If ...
electric and magnetic forces
electric and magnetic forces

... In this apparatus has the same essential features as the display tubes in such devices as oscilloscopes, computer monitors, and televisions. For the electric deflection (Part B) and electric with magnetic deflection (Part C) experiments high voltage applied to the accelerating electrode is the same ...
Nature of Inertia forces
Nature of Inertia forces

Design of Optimal Degaussing Electronics for Ring
Design of Optimal Degaussing Electronics for Ring

... a vital role. Gyro is one of the major parts of the space vehicle. Gyro is used to measure the rotational rate of space vehicles. One of the laser technologies used in gyro is ring laser gyros. Ring laser gyros are effective tools for large scale geodetic surveying at a high level of accuracy. They ...
Document
Document

Plasma transport across magnetic field lines in low
Plasma transport across magnetic field lines in low

Name Date Per ______ Physics – Std 5e: Electrostatics and
Name Date Per ______ Physics – Std 5e: Electrostatics and

Lecture 21: Mean Field Theory of Ferromagnetism
Lecture 21: Mean Field Theory of Ferromagnetism

... moments of partially filled shells in insulators containing transitional metal ions, conduction electrons) do not interact with each other The assumption about noninteracting magnetic moments must be dropped to describe variety of phenomena caused by magnetic interactions. For instance, some materia ...
< 1 ... 376 377 378 379 380 381 382 383 384 ... 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