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diffusion-transfer processor - translation to russian
![Animation of sheet forming process using diffusion welding (see also [[hydroforming]]).](https://commons.wikimedia.org/wiki/Special:FilePath/Output 9GbY2F.gif?width=200 "Animation of sheet forming process using diffusion welding (see also [[hydroforming]]).")
общая лексика
диффузионная сварка
![In 1996, Dutchman [[Edgar Davids]] was the first high-profile player to move on a free transfer via the [[Bosman ruling]].](https://commons.wikimedia.org/wiki/Special:FilePath/Edgar Davids.jpg?width=200 "In 1996, Dutchman [[Edgar Davids]] was the first high-profile player to move on a free transfer via the [[Bosman ruling]].")
![[[John Hartson]] failed medical tests which led to the shelving of three potential transfers in 2000.](https://commons.wikimedia.org/wiki/Special:FilePath/Hartson, John.jpg?width=200 "[[John Hartson]] failed medical tests which led to the shelving of three potential transfers in 2000.")
![Bayern Munich]] from [[RB Leipzig]] for a world record-breaking fee of €25 Million in 2021.](https://commons.wikimedia.org/wiki/Special:FilePath/Julian Nagelsmann 2020.jpg?width=200 "Bayern Munich]] from [[RB Leipzig]] for a world record-breaking fee of €25 Million in 2021.")
![[[Neymar]] (right) and [[Kylian Mbappé]] (left) are the two most expensive association football transfers.](https://commons.wikimedia.org/wiki/Special:FilePath/Mbappe Messi Neymar.jpg?width=200 "[[Neymar]] (right) and [[Kylian Mbappé]] (left) are the two most expensive association football transfers.")
![Barcelona]] in 2013 became the subject of investigation.](https://commons.wikimedia.org/wiki/Special:FilePath/Neymar Barcelona presentation 1.jpg?width=200 "Barcelona]] in 2013 became the subject of investigation.")
![[[Zinedine Zidane]] was the most expensive player in the world for eight years.](https://commons.wikimedia.org/wiki/Special:FilePath/Zidane Zizu.jpg?width=200 "[[Zinedine Zidane]] was the most expensive player in the world for eight years.")
Definition
Wikipedia
The diffusion of plasma across a magnetic field was conjectured to follow the Bohm diffusion scaling as indicated from the early plasma experiments of very lossy machines. This predicted that the rate of diffusion was linear with temperature and inversely linear with the strength of the confining magnetic field.
The rate predicted by Bohm diffusion is much higher than the rate predicted by classical diffusion, which develops from a random walk within the plasma. The classical model scaled inversely with the square of the magnetic field. If the classical model is correct, small increases in the field lead to much longer confinement times. If the Bohm model is correct, magnetically confined fusion would not be practical.
Early fusion energy machines appeared to behave according to Bohm's model, and by the 1960s there was a significant stagnation within the field. The introduction of the tokamak in 1968 was the first evidence that the Bohm model did not hold for all machines. Bohm predicts rates that are too fast for these machines, and classical too slow; studying these machines has led to the neoclassical diffusion concept.
