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fusión de un reactor - перевод на Английский
.png?width=200 "'''Figure 6''': Non-thermalized plasma energy distribution inside a polywell.<ref>\"A biased probe analysis of potential well formation in an electron only, low beta Polywell magnetic field\" Physics of Plasma</ref> It is argued that the region of unmagnetized space leads to electron scattering, this leads to a monoenergetic distribution with a cold electron tail. This is supported by 2 dimensional particle-in-cell simulations.")
![The [[nuclear binding energy]] curve. The formation of nuclei with masses up to [[iron-56]] releases energy, as illustrated above.](https://commons.wikimedia.org/wiki/Special:FilePath/Binding energy curve - common isotopes.svg?width=200 "The [[nuclear binding energy]] curve. The formation of nuclei with masses up to [[iron-56]] releases energy, as illustrated above.")
![The [[CNO cycle]] dominates in stars heavier than the Sun.](https://commons.wikimedia.org/wiki/Special:FilePath/CNO Cycle.svg?width=200 "The [[CNO cycle]] dominates in stars heavier than the Sun.")
![The [[proton–proton chain]] reaction, branch I, dominates in stars the size of the Sun or smaller.](https://commons.wikimedia.org/wiki/Special:FilePath/Fusion in the Sun.svg?width=200 "The [[proton–proton chain]] reaction, branch I, dominates in stars the size of the Sun or smaller.")
![The [[electrostatic force]] between the positively charged nuclei is repulsive, but when the separation is small enough, the quantum effect will tunnel through the wall. Therefore, the prerequisite for fusion is that the two nuclei be brought close enough together for a long enough time for quantum tunneling to act.](https://commons.wikimedia.org/wiki/Special:FilePath/Nuclear fusion forces diagram.svg?width=200 "The [[electrostatic force]] between the positively charged nuclei is repulsive, but when the separation is small enough, the quantum effect will tunnel through the wall. Therefore, the prerequisite for fusion is that the two nuclei be brought close enough together for a long enough time for quantum tunneling to act.")
![The ''[[Tokamak à configuration variable]]'', research fusion reactor, at the [[École Polytechnique Fédérale de Lausanne]] (Switzerland).](https://commons.wikimedia.org/wiki/Special:FilePath/TCV vue gen.jpg?width=200 "The ''[[Tokamak à configuration variable]]'', research fusion reactor, at the [[École Polytechnique Fédérale de Lausanne]] (Switzerland).")
![Diagrama que muestra la nomenclatura de los cambios de estado de acuerdo a la [[entalpía]].](https://commons.wikimedia.org/wiki/Special:FilePath/Phase change - en es.svg?width=200 "Diagrama que muestra la nomenclatura de los cambios de estado de acuerdo a la [[entalpía]].")
Википедия
The polywell is a design for a fusion reactor based on two ideas: heating ions by concentrating (-) charge to accelerate the ions and trapping a diamagnetic plasma inside a cusp field.
This kind of plasma trap is based on the idea that a plasma will create its own magnetic field that rejects the outside field. That is not common behavior for a fusing plasma. A similar trapping concept was tested by the Lockheed-Martin high beta fusion reactor team, which tried to hold a plasma in a similar way.
The Polywell attempts to heat plasma by creating a negative voltage, which attracts positive ions. Like a fusor, as the ions accelerate towards the negative center, their kinetic energy rises. Ions that collide at high enough energies can fuse. But getting this heating approach to work means the Polywell must also concentrate negative charge, which breaks the quasi-neutral assumption.
