• 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 6: Complex Electrical Circuits
Lab 6: Complex Electrical Circuits

... along an equipotential surface (in 3 dimensions). If no work is done, then the potential must be the same everywhere. Clearly there must be zero electric force in the direction of motion along an equipotential. This is all you need to know about electric fields and potentials to begin the experiment ...
Electric Charge and Electric Field
Electric Charge and Electric Field

Taming instability of magnetic field in chiral medium
Taming instability of magnetic field in chiral medium

Dispersion relations for electromagnetic waves in a dense
Dispersion relations for electromagnetic waves in a dense

Why quantum field theory?
Why quantum field theory?

Chapter-24
Chapter-24

Lectures in Physics, summer 2008/09 3
Lectures in Physics, summer 2008/09 3

Biot – Savart Law
Biot – Savart Law

Behavior of Charged Particles in a Biological Cell
Behavior of Charged Particles in a Biological Cell

Light And Telescopes
Light And Telescopes

Quanta and Waves - Calderglen High School
Quanta and Waves - Calderglen High School

... theoretical problems associated with matter on the atomic scale could not be explained by classical physics. During the next three decades, a new theory was developed to explain the behaviour of tiny particles in a range of phenomena such as blackbody radiation, the photoelectric effect, atomic spec ...
Chapters 16 and 17
Chapters 16 and 17

Section 15.3
Section 15.3

Misconception about Quantum Physics slides
Misconception about Quantum Physics slides

Van Wezel_DEF.indd
Van Wezel_DEF.indd

... that is of the order of the inverse gravitational self energy of the difference between the superposed mass distributions [26]. The typical collapse time thus calculated turns out to be extremely large for all quantum mechanical systems that have been studied experimentally, and extremely small for a ...
Electric Fields
Electric Fields

Magnetism
Magnetism

Review of Quantum Mechanics
Review of Quantum Mechanics

x - UW Canvas
x - UW Canvas

Lecture11,ch6
Lecture11,ch6

PHY 220 GENERAL PHYSICS II / 3 credits. Study of electricity
PHY 220 GENERAL PHYSICS II / 3 credits. Study of electricity

... (i) Ability to understand and mathematically analyze the connection between electric potential and electric field in the case of potentials which vary linearly with position. (j) Ability to obtain the capacitance of a system from fundamental considerations and to expand this to cover linear dielectr ...
2011 Take Home Electric Field Gauss` Law AP
2011 Take Home Electric Field Gauss` Law AP

Lamb shift
Lamb shift

Lab 8 Motion of Electrons in Electric and Magnetic Fields
Lab 8 Motion of Electrons in Electric and Magnetic Fields

... Leave the horizontal deflection plates and the coils unconnected. Connect also the digital voltmeter to read the deflection voltage (note that Fig. 5 shows the voltmeter connected to the coils, which will be the case in experiment B). Using the knob on the 30V power supply, vary the deflection volta ...
Magnetic Fields
Magnetic Fields

< 1 ... 299 300 301 302 303 304 305 306 307 ... 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