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... Example: Moving a point charge of 2.3 x 10-19 Coulombs between points A and B in an electric field requires 4.2 x 10-18 joules of energy. What is the potential difference between these points? ...
SI Physics 221
SI Physics 221

Motion of a charged particle in a magnetic field
Motion of a charged particle in a magnetic field

College Physical Science Chapter 9 Assignment MAGNETIC
College Physical Science Chapter 9 Assignment MAGNETIC

... 4. What is the shape of a magnetic field about an electric current when the direction of the current is reversed? 6. Why is the magnetic field strength inside a current carrying loop of wire greater than the field strength about a straight section of wire? MOTORS- read pg. 215-220 7. What relative d ...
Moving Charges and Magnetism
Moving Charges and Magnetism

... Direction of m is given by the right – hand thumb rule: curl and palm of your right hand along the loop with the fingers pointing in the direction of the current. The thumb sticking out gives the direction of ...
Chapter 17
Chapter 17

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Magnetism & electromagnetic

... We have seen how electricity can produce a magnetic field, but a magnetic field can also produce electricity! How? What is electromagnetic induction? Moving a loop of wire through a magnetic field produces an electric current. This is electromagnetic induction. ...
Recitation Week 7
Recitation Week 7

... Problem 27.30. A particle with initial velocity v0 = 5.85 · 103 m/sĵ enters a region of uniform electric and magnetic fields. The magnetic field in the region is B = −(1.35 T)k̂. Calculate the magnitude and direction of the electric field in the region if the particle is to pass through undeflected ...
Semester exam chapter 7. PHYS4315
Semester exam chapter 7. PHYS4315

... b. Show that the magnetic flux through a perfectly conducting loop is constant. A superconductor is a perfect conductor with the additional property that the (constant) B inside is in fact zero. (This “flux exclusion” is known as the Meissner effect. c. Show that the current in a superconductor is c ...
Home Work Problem Set 11
Home Work Problem Set 11

Accelerating Charge Through A Potential Difference
Accelerating Charge Through A Potential Difference

Homework No. 05 (Fall 2014) PHYS 520A: Electromagnetic Theory I
Homework No. 05 (Fall 2014) PHYS 520A: Electromagnetic Theory I

Q: A 1140nF capacitor with circular parallel plates 1
Q: A 1140nF capacitor with circular parallel plates 1

Lecture 16 - UConn Physics
Lecture 16 - UConn Physics

homework 2, due October 3rd
homework 2, due October 3rd

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Chapter 20 EM Induction worksheet

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Unit 4 Day 4 – Electron Properties & Hall Effect

Document
Document

Consider the following solution to the hydrogen atom problem
Consider the following solution to the hydrogen atom problem

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Week 12

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Part II
Part II

... Citation: “For their discovery of a new form of quantum fluid with fractionally charged excitations” • Störmer & Tsui made the discovery in 1982 in an experiment using extremely powerful magnetic fields & low temperatures. Within a year of the discovery Laughlin had succeeded in explaining their res ...
Chapters 21-29
Chapters 21-29

Magnetic Fields VI Name: ____________________
Magnetic Fields VI Name: ____________________

... everywhere within R2 there is a uniform mangetic field B2 = 75 mT into the page. Both fields are decreasing at a rate of 8.50 mT/s (i.e., this number equals –dB/dt). Calculate the integral E   E  dl (which equals a voltage) for each of the three given paths. Path 3 Path 2 R1 ...
May 2001
May 2001

... Problem In this problem, we investigate the effect of electromagnetic waves traveling through a gas of charged particles. This can happen when there is radio emission from a pulsar, and these signals propagate through clouds of charged particles in deep space before being detected on Earth. A linear ...
Charged Particle in an Electromagnetic Field
Charged Particle in an Electromagnetic Field

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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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