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Static Magnetic Fields
Static Magnetic Fields

B = 1.2 T q, m proton: m = 1.67 x 10 kg q = e = 1.6 x 10 C v0 = 2 x 10
B = 1.2 T q, m proton: m = 1.67 x 10 kg q = e = 1.6 x 10 C v0 = 2 x 10

Training Exam based on S13 Phys 1220 ______ name
Training Exam based on S13 Phys 1220 ______ name

Study Guide for Part Three
Study Guide for Part Three

... 23) An electron is moving East with an initial speed of 3x104 m/s through a magnetic field directed up of strength 52 Gauss. a) What is the magnitude and direction of the magnetic force on the electron? b) What is the magnitude of the acceleration of the electron? 24) A certain mass spectrometer has ...
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Q- Three point charges are aligned along the x

Inner Magnetosphere
Inner Magnetosphere

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2nd trimester groupwork #1 Group 7A

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21201t3

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22-1,2,3,4

KTH | MH1026 Materials Physics 6.0 credits
KTH | MH1026 Materials Physics 6.0 credits

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Lecture 14. Magnetic Forces on Currents. Outline: Hall Effect.
Lecture 14. Magnetic Forces on Currents. Outline: Hall Effect.

... Direct Current Motor C. tends to make the loop rotate around its axis. How can we realize this situation? – By changing the direction of current once per period of rotation. ...
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III-2

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24-2: Electric potential energy

Purdue University PHYS221 EXAM I September 30,2003
Purdue University PHYS221 EXAM I September 30,2003

... Two charged particles move in the same direction with respect to the same magnetic field. Particle 1 travels three times faster than particle 2. However, each particle experiences a magnetic force of the same magnitude. Find the ratio q1/q2 of the magnitudes of the charges.(5 points) ...
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Exam-Pre Board-1 st

D NAME: 1. What is the eigenvalue of Lz for Ψ if the eigenval
D NAME: 1. What is the eigenvalue of Lz for Ψ if the eigenval

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... magnetic fields and their effects on moving charges  state the rules explaining how magnetic poles interact with each other  describe and illustrate the direction of the magnetic field lines for a permanent magnet  use the right-hand rule to determine the magnetic field direction for a current-ca ...
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Homework 12

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Motion in One Dimension

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Review 16 and 17

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MCQ based on activity for 10 CBSE Magnetic effect of current
MCQ based on activity for 10 CBSE Magnetic effect of current

... no definite direction. Another bar P-Q of the same metal always comes to rest with end P pointing North. What is the result if the two bars are brought near one another? A. P attracts X but repels Y. B. P neither attracts nor repels X. C. P attracts X but Q repels Y. D. P and Q both attract X. 15) ...
Electric Potential - McMaster Physics and Astronomy
Electric Potential - McMaster Physics and Astronomy

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Tight-binding model
Tight-binding model

... In our naive derivation, we did not treat the Lorentz transformation between the lab frame and the electron’s rest frame completely correctly. An electron moving in an electric field that has a component perpendicular to the electron’s velocity describes a curved trajectory. The transformation betwe ...
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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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