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The Force and Nature of Magnetism
The Force and Nature of Magnetism

... Magnetic resonance imaging machines were invented by Sir Peter Mansfield in the 1970’s as a way to obtain two-dimensional images of the human body. An MRI machine uses a very powerful manmade magnetic field 40,000 times stronger than the Earth's to look at the tissues and organs in the human body. A ...
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... fraction of one percent of the main field, and amounts to only a few minutes in declination. Over regions where igneous rocks are at or near the surface, anomalies in declination often reach tens of minutes, occasionally as much as one or two degrees. In some places magnetite has been concentrated t ...
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... A classic demonstration illustrating eddy currents is performed by dropping a permanent magnet inside a conducting cylinder. The magnet does not go into free fall. Instead it reaches terminal velocity and can take a few seconds to drop a length of about a meter. Suppose the mass of the magnet is 70 ...
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Episode 411: Describing magnetic fields

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Word version of Episode 411

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2010 Japan Prizes Awarded to Prof. Shun

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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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