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Magnetism and Uses
Magnetism and Uses

... Moving coil of wire within a magnetic field induces a current in the wire Produces AC because of the switch in direction of magnetic fields in the permanent magnets Faraday’s Law of Induction – faster the solenoid turns in the magnetic field the higher the voltage Turbine forced to turn by wind, fal ...
Revisiting moving electric charges
Revisiting moving electric charges

... A 20 μF parallel plate capacitor stores 300 μC of charge. The plates are 6 cm apart. An electron enters the region between the plates along the midpoint with a speed of 1 x 106 m/s as shown. What is the magnitude and direction of the force that acts on the electron (Neglect gravity). Sketch the path ...
Paper - Kendriya Vidyalaya IIT Chennai
Paper - Kendriya Vidyalaya IIT Chennai

Possible Topics for the Final Project Taken with slight modification
Possible Topics for the Final Project Taken with slight modification

Cyclotron powerpoint lecture
Cyclotron powerpoint lecture

... • After entering the second magnetic field, the ions move in a semicircle of radius r before striking a detector at P • If the ions are positively charged, they deflect to the left • If the ions are negatively charged, they deflect to the right • mv2/R=qvB, therefore m/q=RB/v ...
ELECTRIC POTENTIAL
ELECTRIC POTENTIAL

SCHRÖDINGER EQUATION FOR A PARTICLE ON A CURVED SPACE AND SUPERINTEGRABILITY
SCHRÖDINGER EQUATION FOR A PARTICLE ON A CURVED SPACE AND SUPERINTEGRABILITY

File
File

... waves. The electromagnetic waves produced are radiated from the spark gap. The detector is held in a position such that the magnetic field produced by the oscillating current is perpendicular to the plane of the coil. The resultant electric field induced by the oscillating magnetic field causes the ...
Slide 1
Slide 1

Given that a bulb is a 2 meters away, how long
Given that a bulb is a 2 meters away, how long

...  E and B field oscillate  E and B are perpendicular to each other and to the direction of propagation  E, B, and Propagation related by Right-hand Rule 2  Travels at the “speed of light” in vacuum, and at ...
General Physics II - Tennessee State University
General Physics II - Tennessee State University

... 15. Three charges are placed as follows along the x and y axes of an xy-coordinate system: q1 = 2.00 µC at x1 = 0 m, q2 = 4.00 µC at x2 = 3.00 m, and q3 = 6.00 µC at y = 4.00 m. What is the electric potential energy of this system of charges? A) -94.2 mJ B) 94.2 mJ C) 0 J D) 90.0 mJ 16. The work don ...
Scientific Poster Example/Template
Scientific Poster Example/Template

2016_Goswami_Partha_physicsgoswami@gmail
2016_Goswami_Partha_physicsgoswami@gmail

Slide 1
Slide 1

12.1: What are electromagnetic waves?
12.1: What are electromagnetic waves?

magnetism
magnetism

... either oscillate current, or push it hard enough to “flip” ...
Document
Document

... inside the powerful magnetic field of the scanner, the average magnetic moment of many protons becomes aligned with the direction of the field. A radio frequency current is briefly turned on, producing a varying electromagnetic field. This electromagnetic field has just the right frequency, known as ...
Special_Relativity_7
Special_Relativity_7

PHYS6520 Quantum Mechanics II Spring 2013 HW #5
PHYS6520 Quantum Mechanics II Spring 2013 HW #5

... matching right and left going waves on the left with a right going wave on the right at x = 0. You’ll need to integrate the Schrödinger equation across x = 0 to match the derivatives. (e) We showed last semester that this potential has one, and only one, bound state. Show that your results for T (k ...
PH504-10-test-Q-and-A
PH504-10-test-Q-and-A

Physics 121 Practice Problem Solutions 09 Magnetic Fields Contents:
Physics 121 Practice Problem Solutions 09 Magnetic Fields Contents:

Ch. 29/30 Practice Test — Solution
Ch. 29/30 Practice Test — Solution

... 5. (e) The magnetic field does no work because the force is always perpendicular to the velocity. 6. (b) ~ = (15 A)(2.0î) m×(30î−40ĵ) mT = [30î×(−40ĵ)] mN = (−1200k̂) mN = (−1.20k̂) N F~B = I~l×B Alternatively, by the right hand rule, F~B points down. Its magnitude equals the area of the ~ whic ...
wavefunction (63) obtained by applying Dirac`s factor
wavefunction (63) obtained by applying Dirac`s factor

pdf x1
pdf x1

...   It applies to any closed path   It applies to any static B field   It is practically useful in symmetric cases ...
•How vision works •What is light •Wavelength and Frequency: c = f λ
•How vision works •What is light •Wavelength and Frequency: c = f λ

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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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