4,427
edits
Scaling law: Difference between revisions
→Confinement time scaling
| Line 38: | Line 38: | ||
<ref name="ITER">[http://dx.doi.org/10.1088/0029-5515/39/12/301 ITER Physics Expert Groups et al, ''ITER Physics Basis, Chapter 1'', Nucl. Fusion '''39''' (1999) 2137] and [http://dx.doi.org/10.1088/0029-5515/39/12/302 Ibid., ''Chapter 2'']</ref> | <ref name="ITER">[http://dx.doi.org/10.1088/0029-5515/39/12/301 ITER Physics Expert Groups et al, ''ITER Physics Basis, Chapter 1'', Nucl. Fusion '''39''' (1999) 2137] and [http://dx.doi.org/10.1088/0029-5515/39/12/302 Ibid., ''Chapter 2'']</ref> | ||
* L-mode scaling | * L-mode scaling | ||
* ELMy H-mode scaling (IPB98(y,2)) | * ELMy [[H-mode]] scaling (IPB98(y,2)) | ||
For stellarators, a similar scaling has been obtained (ISS). | For stellarators, a similar scaling has been obtained (ISS). | ||
| Line 60: | Line 60: | ||
When α = 0, the scaling is said to be of the Bohm type, and when α = 1, of the gyro-Bohm type. | When α = 0, the scaling is said to be of the Bohm type, and when α = 1, of the gyro-Bohm type. | ||
The ELMy H-mode scaling is of the gyro-Bohm type. | The ELMy [[H-mode]] scaling is of the gyro-Bohm type. | ||
Gyro-Bohm scaling is what one would expect for diffusive transport based on a diffusive scale length proportional to ρ<sub>i</sub> (the ion gyroradius). | Gyro-Bohm scaling is what one would expect for diffusive transport based on a diffusive scale length proportional to ρ<sub>i</sub> (the ion gyroradius). | ||