| Presentation/ MP number |
First Author |
Title | Requested run days | Priority | Special resources | Comments |
| Ideas 2007 MHD topical group presentations | ||||||
| 2007-401 | Wolfe | Effect of non-resonant non-axisymmetric fields on locked mode threshold | 1 (or 1/2 + 1/2) | M | ||
| 2007-402 | Wolfe | Reverse helicity (I anti-parallel to B) locked mode threshold study | 0.5-3 | L | Reverse B (but not PF) | Depends on outcome of 2007-401 |
| 2007-403 | Wolfe | Seeding NTM's using A-coil induced locked mode | 1-2 | - | Cryopump; max P_icrf | Combine with 2007-405 |
| 2007-404 | Wolfe | LHCD effect on tearing mode stability | 1+1+2 | H (1) | LHCD | |
| 2007-405 | Snipes | NTM Stability at Low Collisionality | 1 | H (1) | Cryopump; high beta_N | Combine with 2007-403 |
| 2007-406 | Snipes | Stable TAE n discrimination with Plasma Rotation | 1 | - | Ohmic H-mode | Combine with 2007-302 or 308 (Transport Ohmic H-modes)? |
| 2007-407 | Snipes | Sensitivity of Stable TAE Damping to Profile Effects | 2 | M | LHCD for 1 of the days | |
| 2007-408 | Snipes | Measurement of LHCD Effects on q(r) Through Stable and Unstable Alfvén Eigenmodes in the Current Flattop | 2 (1 stable, 1 unstable) | H (1) | LHCD | Combine "stable" days of 408 and 409 |
| 2007-409 | Snipes | Measurement of LHCD Effects on q(r) Through Stable and Unstable Alfvén Eigenmodes in the Current Rise | 2 (1 stable, 1 unstable) | H (1) | LHCD | |
| 2007-410 | Porkolab | Evolution of AT target plasmas and Alfven cascades during the current ramp and beyond with LHCD q-profile control | 0-1 | H (1) | LHCD | Combine with "unstable" day of 409 |
| 2007-411 | Edlund | Studies of Alfvén eigenmode excitation during the sawtooth cycle in low density plasmas | 0-1 | H (1) | Pellets? | Thesis related; Incorporate 2007-1110 into this. |
| 2007-412 | Sears | Damping rate of Toroidal Alfvén Eigenmodes at the threshold of stability in the presence of ICRF heated fast ions | 2 | H (1.5) | Thesis related; later in campaign is desirable | |
| 2007-413 | Granetz | Try using FRCECE to see TAE mode structure | 0 (all piggyback) | H (0) | ||
| 2007-414 | Granetz | Real-time detection and gas jet mitigation of locked mode disruptions | 0.5-1 | H (1) | DPCS programming | |
| 2007-415 | Granetz | Determine minimum amount of gas required with Ar/He mixed gas jet disruption mitigation | 1 | H (1) | ||
| 2007-416 | Granetz/Wesley | Disruption mitigation using a deuterium gas jet | 1 | - | combine with 2007-418 | |
| 2007-417 | Reinke | Using fast, 2D bolometry to diagnose disruption mitigation radiation | 0.5 dedicated | M | 0.5 days of pure Ar | Also piggyback on gas jet disruption runs |
| 2007-418 | Whyte | Disruption mitigation & opacity studies using D2 massive gas injection | 0.5 | H (0.5) | Combine 2007-416 (Wesley) with 2007-418 (Whyte). | |
| 2007-419 | Whyte | ELM mitigation and pacing with impurity injection | 0 (effectively) | L | special gases and injection hardware | Not feasible this year |
| Transferred from other Ideas 2007 topical groups | ||||||
| 2007-910 | Hender | Joint experiments with JET on non-resonant n=2 magnetic braking | 1/2 + 1/2 | H (1) | medium
priority in Integrated scenarios/H-mode baseline topical group Proof-of-principle combined with 2007-911. |
|
| Open MHD miniproposals | ||||||
| MP 395 | Granetz | Dimensionless comparison of NTM thresholds | 1 | M | High beta_N | medium priority in Integrated scenarios/H-mode baseline topical group |
| MP 407 | Lao | Effects of 3D Error Fields on Magnetic Surfaces | 1 | M | ||
| MP 432 | Granetz | TAEs and RF tail losses | 1 | M | CNPA desirable | medium priority in Integrated scenarios/H-mode baseline topical group |