Ion Temperature Gradient instability: Difference between revisions

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The ion temperature gradient (ITG) instability is a microinstability in tokamaks relevant to turbulence and the associated anomalous transport.
The ion temperature gradient (ITG) instability<ref> P. N. Guzdar, Liu Chen, W. M. Tang and P. H. Rutherford, ''Ion‐temperature‐gradient instability in toroidal plasmas'' [[doi:10.1063/1.864182|Phys. Fluids '''26''' (1983) 673]]</ref> is a microinstability in [[tokamak]]s relevant to turbulence and the associated [[anomalous transport]].


The instability occurs due to the nature of Grad-B drift. The Grad-B drift velocity of a particle (caused by a gradient in the magnetic field) is proportional to the particle's kinetic energy. Hotter particles drift further than colder particles.
The instability occurs due to the nature of Grad-B drift. The Grad-B drift velocity of a particle (caused by a gradient in the magnetic field) is proportional to the particle's kinetic energy. Hotter particles drift further than colder particles.


Hence, if a temperature gradient is aligned with a magnetic field gradient (as occurs in a tokamak), particles in the hotter region will drift further. If there is a perturbation in the temperature gradient, then the difference in drift velocities will create charge separation. The charge separation creates a electric field. This electric field creates an ExB drift which increases the perturbation's amplitude. The positive-feedback nature of this loop leads to exponential growth of the instability.
Hence, if a temperature gradient is aligned with a magnetic field gradient (as occurs in a tokamak), particles in the hotter region will drift further. If there is a perturbation in the temperature gradient, then the difference in drift velocities will create charge separation. The charge separation creates an electric field. This electric field creates an <math>E\times B</math> drift which increases the perturbation's amplitude. The positive-feedback nature of this loop leads to exponential growth of the instability.


See the figure to see the geometric setup.
Note that if the temperature gradient is anti-parallel to the magnetic field gradient, the <math>E\times B</math> drift will suppress the perturbation rather than increase it.  This situation occurs on the inner, "good-curvature" side of the tokamak.


Note that if the temperature gradient is anti-parallel to the magnetic field gradient, the ExB drift will suppress the perturbation rather than increase it.  This situation occurs on the inner, "good-curvature" side of the tokamak.
See the figure for a graphical explanation.


[[File:ITG.eps]]
[[File:ITG.png|600px|thumb|center|ITG mechanism]]
 
== See also ==
 
* [[Plasma instability]]
 
== References ==
<references/>

Latest revision as of 19:21, 28 June 2021

The ion temperature gradient (ITG) instability[1] is a microinstability in tokamaks relevant to turbulence and the associated anomalous transport.

The instability occurs due to the nature of Grad-B drift. The Grad-B drift velocity of a particle (caused by a gradient in the magnetic field) is proportional to the particle's kinetic energy. Hotter particles drift further than colder particles.

Hence, if a temperature gradient is aligned with a magnetic field gradient (as occurs in a tokamak), particles in the hotter region will drift further. If there is a perturbation in the temperature gradient, then the difference in drift velocities will create charge separation. The charge separation creates an electric field. This electric field creates an drift which increases the perturbation's amplitude. The positive-feedback nature of this loop leads to exponential growth of the instability.

Note that if the temperature gradient is anti-parallel to the magnetic field gradient, the drift will suppress the perturbation rather than increase it. This situation occurs on the inner, "good-curvature" side of the tokamak.

See the figure for a graphical explanation.

ITG mechanism

See also

References

  1. P. N. Guzdar, Liu Chen, W. M. Tang and P. H. Rutherford, Ion‐temperature‐gradient instability in toroidal plasmas Phys. Fluids 26 (1983) 673