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Tutorial 3 Magnetostatics
Tutorial 3 Magnetostatics

... field. The magnetic flux density with 3.5 T experiences a magnetic force of magnitude 2x10-13 N. Determine the angle between the magnetic field and proton’s velocity? Biot- Savart Law Q5. The metal niobium becomes a superconductor with the zero electrical resistance when it is cooled to below 9 K, b ...
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... Here we see that the FIELD is directly related to the CHARGE and inversely related to the square of the displacement. The only difference in the case of the B-Field is that particle MUST be moving and the vectors MUST be perpendicular. ...
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Magnetic flux - Purdue Physics

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PhD position: Dynamic Nuclear Polarization using Electron-Nuclear Double Resonance

... Electron spins are more easily polarized because their magnetic moments are around 1,000 times greater than those of nuclear spins. For the conditions of interest this provides around 1,000 times more electron spin polarization than nuclear spin polarization. If we can transfer all of this to the nu ...
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Electron Spin Resonance

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HW 6 Due on Mar 11 5.9, 5.10, 6.2, 6.3, 6.4, 6.5 For 5.9, it was

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Nguyễn Văn Đồng1, Phạm Thị Lý Thu1, Phạm Thị Hương1,Trần

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< 1 ... 165 166 167 168 169 170 171 172 173 ... 178 >

Magnetochemistry



Magnetochemistry is concerned with the magnetic properties of chemical compounds. Magnetic properties arise from the spin and orbital angular momentum of the electrons contained in a compound. Compounds are diamagnetic when they contain no unpaired electrons. Molecular compounds that contain one or more unpaired electrons are paramagnetic. The magnitude of the paramagnetism is expressed as an effective magnetic moment, μeff. For first-row transition metals the magnitude of μeff is, to a first approximation, a simple function of the number of unpaired electrons, the spin-only formula. In general, spin-orbit coupling causes μeff to deviate from the spin-only formula. For the heavier transition metals, lanthanides and actinides, spin-orbit coupling cannot be ignored. Exchange interaction can occur in clusters and infinite lattices, resulting in ferromagnetism, antiferromagnetism or ferrimagnetism depending on the relative orientations of the individual spins.
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