• 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
4. Electric Fields in Matter
4. Electric Fields in Matter

...  Pabove  Pbelow ...
Tuesday, Sept. 13, 2011
Tuesday, Sept. 13, 2011

... –  The electric force is a conservative force. –  Thus, the mechanical energy (K+U) is conserved under this force. –  The charged object has only the electric potential energy at the positive plate. –  The electric potential energy decreases and –  Turns into kinetic energy as the electric force wor ...
quantum physics - Enggphysicsvenkat
quantum physics - Enggphysicsvenkat

y - Journal des Sciences
y - Journal des Sciences

... factors on solar cells have been proposed in one dimensional study. In this work, we propose a three dimensional study of bifacial solar cell under intense light concentration (more than 50 suns) and under external variable magnetic field. The calculations were carried out in the case of a polycryst ...
Thermal and vacuum friction acting on rotating particles
Thermal and vacuum friction acting on rotating particles

1. What is the equivalent capacitance between points a and b? All
1. What is the equivalent capacitance between points a and b? All

... 1. What is the equivalent capacitance between points a and b? All capacitors are 3.0 PF- ...
Life after Charge Noise: An Introduction to the Transmon Qubit
Life after Charge Noise: An Introduction to the Transmon Qubit

... Yu. Makhlin, G. Schön, and A. Shnirman, Rev. Mod. Phys. 73, 357 (2001) M. H. Devoret, A. Wallraff and J. M. Martinis, cond-mat/0411172 (2004) J. Q. You and F. Nori, Phys. Today, Nov. 2005, 42 J. Clarke, F. K. Wilhelm, Nature 453, 1031 (2008) ...
Restructuring the introductory electricity and magnetism course
Restructuring the introductory electricity and magnetism course

Magnetism MC practice problems
Magnetism MC practice problems

Theory of shot noise in high-current space-charge-limited
Theory of shot noise in high-current space-charge-limited

TRImP Trapped Radioactive Isotopes
TRImP Trapped Radioactive Isotopes

Time reversal (reversal of motion)
Time reversal (reversal of motion)

Chapter 6. Magnetostatic Fields in Matter
Chapter 6. Magnetostatic Fields in Matter

... Consider a rectangular current loop, with sides s1 and s2, located in a uniform magnetic field, pointing along the z axis. The magnetic dipole moment of the current loop makes an angle q with the z axis (see Figure 6.1a). The magnetic forces on the left and right sides of the current loop have the s ...
Conduction electrons propagate diffusively in the system: bumping
Conduction electrons propagate diffusively in the system: bumping

ELECTRIC CHARGE, CONDUCTORS AND INSULATIONS
ELECTRIC CHARGE, CONDUCTORS AND INSULATIONS

Acoustic Analog to Quantum Mechanical Level Splitting
Acoustic Analog to Quantum Mechanical Level Splitting

No Slide Title
No Slide Title

Jan. 17 notes - Review of electrostatics pt. 1
Jan. 17 notes - Review of electrostatics pt. 1

... Free electrons inside the conductor will quickly move around and redistribute themselves in such a way that they will cancel out the field in the conductor (as the electrons move they leave behind positively charged atoms). Very quickly the field inside the conductor will become zero. There is also ...
7.6 - Millikan Oil Drop Experiment
7.6 - Millikan Oil Drop Experiment

Lesson #3 – Gauss` Law
Lesson #3 – Gauss` Law

... (Cylindrical objects  use cylindrical surface) (Spherical objects  use spherical surface) (Plate objects  use plane surface) ...
CYC69H07
CYC69H07

Seasonal polar cap radiation zones in dayside magnetosphere G. Pugacheva
Seasonal polar cap radiation zones in dayside magnetosphere G. Pugacheva

Jackson 1.9 Homework Solution
Jackson 1.9 Homework Solution

Document
Document

... E. Infinite ...
Book 2 - San Diego Mesa College
Book 2 - San Diego Mesa College

< 1 ... 284 285 286 287 288 289 290 291 292 ... 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