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Magnetic Force on a current-carrying Wire
Magnetic Force on a current-carrying Wire

... magnetic force FB . Since electric current consists of a collection of charged particles in motion, when placed in a magnetic field, a current-carrying wire will also experience a magnetic force. Consider a long straight wire suspended in the region between the two magnetic poles. The magnetic field ...
a) A b) B c) C
a) A b) B c) C

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N/Z = 2, 8, 20, 28, 50, 82, 126

1 magnetic induction - Purdue Physics
1 magnetic induction - Purdue Physics

key - circuits 7
key - circuits 7

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... Zeeman effect (1896) – Nobel prize in physics (1902) Nature 55, 347 (1897) The effect of magnetisation on the nature of light emitted by a substance ...
NA 2nd Semester Review Regular Physics No Ans
NA 2nd Semester Review Regular Physics No Ans

TAP 406-1: Demonstration – electric field lines
TAP 406-1: Demonstration – electric field lines

TAP 406-1: Demonstration – electric field lines
TAP 406-1: Demonstration – electric field lines

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ELECTRIC POTENTIAL-ENERGY (U)

Energy Level diagram for a spin-1/2 nucleus as a function of
Energy Level diagram for a spin-1/2 nucleus as a function of

... Repeat the above calculation for 1H which has a megnetogyric ratio of 26,753 rad/secG. Calculate the energy level diagram and precession frequencies for 11.7 and 7 T. What are the operating frequencies, Larmor frequencies, of these fields? BmIrad/sec G)][11.7 T][10000 G/T][mI]/[2* ...
Physics 08-04 Conductors in Equilibrium and Applications
Physics 08-04 Conductors in Equilibrium and Applications

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PHYSICS 241 TEST 1 Monday, February 17, 2003

... 3.) Charges Q1 = +10nC and Q2 = -30nC are placed on the x axis at x = 0 and x = 50 cm, respectively. What is the net electric flux, in Nm2/C, through a spherical surface of radius r = 40 cm centered on the origin of coordinates? a) b) c) d) e) ...
Physics Practice Paper 1 - TWGHs. Kap Yan Directors` College
Physics Practice Paper 1 - TWGHs. Kap Yan Directors` College

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PHYSICS 7

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Chapter 6. Maxwell Equations, Macroscopic Electromagnetism

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Magnetic Materials

... Motion of Charges in B Fields If a charged particle is moving perpendicular to a uniform magnetic field, its trajectory will be a circle because the force F=qvB is always perpendicular to the motion, and therefore centripetal. ...
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AKSHAYA COLLEGE OF ENGINEERING AND TECHNOLOGY

... (ii) A capacitor consists of squared two metal plates each 100 cm side placed parallel and 2 mm apart. The space between the plates is filled with a dielectric having a relative permittivity of 3.5. A potential drop of 500 V is maintained between the plates. Calculate i) the capacitance, ii) the cha ...
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Conductance quantization and quantum Hall effect
Conductance quantization and quantum Hall effect

16-3 Electrical Potential Difference
16-3 Electrical Potential Difference

... Remember, the term “work” can be replaced with the term “energy,” because to store energy in, or give energy to, an object, work must be done. Therefore, potential difference can also be defined as the electrical potential energy per unit test charge. Voltage is often used to mean potential differen ...
Homework No. 05 (2014 Fall) PHYS 320: Electricity and Magnetism I
Homework No. 05 (2014 Fall) PHYS 320: Electricity and Magnetism I

Test3_11_key
Test3_11_key

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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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