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SMART Notebook
SMART Notebook

EE3321 ELECTROMAGENTIC FIELD THEORY
EE3321 ELECTROMAGENTIC FIELD THEORY

Q - Moodle NTOU
Q - Moodle NTOU

CT_electrostatics
CT_electrostatics

... 1. Yes, we must move the particles farther apart. 2. Yes, we must move the particles closer together. 3. No, at any distance ...
Name: Electrostatic Potential and Electric Energy – Practice 1
Name: Electrostatic Potential and Electric Energy – Practice 1

Quantum Mechanics_Gauss`s law for magnetism
Quantum Mechanics_Gauss`s law for magnetism



... So the work done on the charges and currents by the fields per unit time will be equal to a decrease of energy stored in the field (first term on the right) and the rate with which energy is transported out of V (2nd term of the right). Note that the 2nd integral is equal to zero if the magnetic fie ...
General Physics II
General Physics II

PPT - LSU Physics & Astronomy
PPT - LSU Physics & Astronomy

Lesson 4: Electric Potential
Lesson 4: Electric Potential

... •For q, instead of coulombs, use units: elementary charges, e the number of ______________________ Using these new units, the potential difference V in: V = W/q ...
Unit I (Magnetism) course notes
Unit I (Magnetism) course notes

The atom in electric field
The atom in electric field

... The exact solution leads to ...
Problem set 2
Problem set 2

... is real, so that we are justified in calling it a phase angle. Here ψn (t) are orthonormal eigenstates of the hamiltonians H(t) for each t with eigenvalues En (t). 2. With the same notation as above, show that Ėn = hψn |Ḣ|ψn i. ...
Chapters 21 - 29 PHYS 2426
Chapters 21 - 29 PHYS 2426

Magnetism
Magnetism

Chapter 31 Faraday`s Law
Chapter 31 Faraday`s Law

Magnetotransport of Topological Insulators
Magnetotransport of Topological Insulators

Reference Frames and Relative Motion Uniform Circular Motion
Reference Frames and Relative Motion Uniform Circular Motion

... N Even an individual electron has a magnetic “dipole”! ...
space charge effects - CERN Accelerator School
space charge effects - CERN Accelerator School

Chapter 20
Chapter 20

... • Electrons in metal are free to move. • The magnetic field is horizontal and to the left. • The ends of the coil are connected to a load such as a light bulb (not shown). See the next slide for questions. © Houghton Mifflin Harcourt Publishing Company ...
Syllabus
Syllabus

... The main objective of this course is to examine the theoretical basis for our present understanding of the structure of matter at the atomic and molecular level. To that end we will review those aspects of quantum mechanics that play the most important role in this understanding. This includes the s ...
Exam 2 Physics 195B (3/14/02)
Exam 2 Physics 195B (3/14/02)

Basics of electrodynamics
Basics of electrodynamics

Electrons
Electrons

Hall Effect - WordPress.com
Hall Effect - WordPress.com

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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).
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