Internal Transport Barrier: Difference between revisions
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The mechanism for the formation of Internal Transport Barriers in magnetically confined plasmas is complex and not fully understood. Probably, it is related to the mechanism for the formation of the [[H-mode]] barrier, involving turbulence suppression by sheared (''E'' × ''B'') flows. | The mechanism for the formation of Internal Transport Barriers in magnetically confined plasmas is complex and not fully understood. Probably, it is related to the mechanism for the formation of the [[H-mode]] barrier, involving turbulence suppression by sheared (''E'' × ''B'') flows. | ||
<ref>[http://link.aip.org/link/?PHPAEN/4/1499/1 K.H. Burrell, ''Effects of E × B velocity shear and magnetic shear on turbulence and transport in magnetic confinement devices'', Phys. Plasmas '''4''' (1997) 1499]</ref> | |||
ITBs are often found to be associated with rational magnetic surfaces. | ITBs are often found to be associated with rational magnetic surfaces. | ||
Revision as of 13:39, 28 August 2009
No generally accepted definition for Internal Transport Barriers (ITBs) exists. Vaguely speaking, the term refers to a radially localized reduction of transport for ions or electrons.
ITBs can be actively produced by modifying the current profile using external means. [1] They are used to improve plasma confinement and stability properties, and to drive additional bootstrap current. Therefore, they are included in some alternative operational scenarios for ITER.
Physical mechanism
The mechanism for the formation of Internal Transport Barriers in magnetically confined plasmas is complex and not fully understood. Probably, it is related to the mechanism for the formation of the H-mode barrier, involving turbulence suppression by sheared (E × B) flows. [2] ITBs are often found to be associated with rational magnetic surfaces.
Factors contributing to the formation of ITBs include: [3]
- Power deposited inside the magnetic surface, and/or pressure gradients
- Magnetic shear and the shape of the rotational transform profile
- MHD activity
- Momentum torques (poloidal or toroidal)
- Enhanced collisionless losses of trapped particles, generating a radial electric field [4]
- Reduced collisional damping, allowing the growth of zonal flows [5]
References
- ↑ R.C. Wolf, Internal transport barriers in tokamak plasmas, Plasma Phys. Control. Fusion 45 (2003) R1-R91
- ↑ K.H. Burrell, Effects of E × B velocity shear and magnetic shear on turbulence and transport in magnetic confinement devices, Phys. Plasmas 4 (1997) 1499
- ↑ J.W. Connor et al, A review of internal transport barrier physics for steady-state operation of tokamaks, Nucl. Fusion 44 (2004) R1-R49
- ↑ U. Stroth et al, Internal Transport Barrier Triggered by Neoclassical Transport in W7-AS, Phys. Rev. Lett. 86 (2001) 5910 - 5913
- ↑ K. Itoh et al, Physics of internal transport barrier of toroidal helical plasmas, Phys. Plasmas 14 (2007) 020702