• 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
T9 Q1-5
T9 Q1-5

Gravitational Waves and Gravitons
Gravitational Waves and Gravitons

Magnetic Force Lab SP222
Magnetic Force Lab SP222

Electron Temperature Effect on Plasma Potential for Different
Electron Temperature Effect on Plasma Potential for Different

Chapter 3
Chapter 3



272 First review
272 First review

... Suppose that it is determined that 10 field lines radiate from the + 2 C charge, then for the – 4 C charge (a) 20 field lines will radiate in (b) 10 field lines will radiate in (c) 20 field lines will radiate out (d) 5 field lines will radiate out (e) 5 field lines will radiate in 12. A certain ph ...
Electromagnetic radiation
Electromagnetic radiation

Exam 1 Solutions
Exam 1 Solutions

... With four charges, there are 6 pairs: 12, 13, 14, 23, 24, 34. Let L be the length of a side. Four pairs (corresponding to the 4 sides) each contribute −kQ 2 / L while the diagonals each contribute kQ 2 / 2L . The total potential energy is thus ...
Statistical Mechanics of Phase Transition
Statistical Mechanics of Phase Transition

Relativity Problem Set 9 - Solutions Prof. J. Gerton October 23, 2011
Relativity Problem Set 9 - Solutions Prof. J. Gerton October 23, 2011

1. dia
1. dia

2 Particle dynamics
2 Particle dynamics

... The particle is called free body if it is no in interaction with any other body or field. Newton’s first law: It is possible to find a reference system in which the free body or particle does not experience acceleration or its speed is constant or zero. This reference system is called inertial syste ...
Chapter 19 Practice
Chapter 19 Practice

... What is the direction of the electric field at the location of the letter “D?” a) perpendicular to the equipotential line marked “D” and directed toward the negative charge closest to it b) parallel to the equipotential line marked “D” and directed toward the location of the letter “C” c) perpendicu ...
R - 核融合科学研究所
R - 核融合科学研究所

High-voltage lines
High-voltage lines

MAT389 Fall 2014, Problem Set 5 (due Oct 23) Holomorphic functions
MAT389 Fall 2014, Problem Set 5 (due Oct 23) Holomorphic functions

... constant. In terms of the three-dimensional picture, we are placing the wire along the z-axis, and r is the radial coordinate in a cylindrical coordinate system. Now think of that same wire inside a cylinder of unit radius and parallel to it. If we keep the surface of the cylinder at a constant valu ...
pisa lecture 3
pisa lecture 3

Physics 9 Fall 2009
Physics 9 Fall 2009

... of electrons turn a 90◦ corner. This can be done with the parallel-plate capacitor shown in the figure. An electron with kinetic energy 3.0 × 10−17 J enters through a small hole in the bottom plate of the capacitor. (a) Should the bottom plate be charged positive or negative relative to the top plat ...
Document
Document

Document
Document

The Electric Dipole - University of Toronto Physics
The Electric Dipole - University of Toronto Physics

LAGRANGIAN FORMULATION OF THE ELECTROMAGNETIC
LAGRANGIAN FORMULATION OF THE ELECTROMAGNETIC

... mz 00 (t) = −∂z U Since free particles are only under the influence of conservative forces, and conservative forces can be written as the negative of the spatial derivative of a scalar potential energy function, the above equations reduce to ma = F Which is just Newton’s second law in vector form. I ...
Supplementary materials
Supplementary materials

Electric Field
Electric Field

< 1 ... 354 355 356 357 358 359 360 361 362 ... 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