Tokamak: TFTR Pulse Number: 91472 Contact: E. Synakowski Institution: PPPL, Princeton University Date of Shot: February 1, 1996 Analysis Code: TRANSP Run number: 91472a02 Analysis Date: August 15, 1997 Assumptions: Zeff profile determined from carbon density profile measured by CXRS, normalized to a single chord- integral VB measurement. Prior to the start of NBI, Ti profile is calculated assuming chii = 15 x neoclassical, which is the value observed in other expts. During NBI, Ti and Vphi are measured by CXRS. Shot Desc.: Supershot to L-mode perturbation caused by carbon bloom event. The bloom starts at about 4.0 seconds, after approximately 30 MJ of beam energy has been deposited in the plasma over a period of 1200 ms of beam injection. During the bloom, the central ion temperature drops a factor of three over a period of ~200-300 msec. Some of this decrease can be attributed directly to increased beam attenuation caused by the higher edge density; beam power delivered to the core decreases 30% after 200 ms and 50% after 300 ms. However, the response of the ion temperature is considerably stronger than would be expected from the decreased core power delivery. Time-dependent transport analysis by TRANSP concludes that the ion thermal diffusivity in the core (r/a = 0.25-0.35) increases about a factor of five by 4.2 seconds, i.e. about 200 ms into the bloom event. Interestingly, the fractional decrease in central ion temperature during the bloom is much greater than the corresponding change in edge ion temperature. Indeed, at 4.2 seconds the edge Ti has hardly changed, while the central ion temperature drops by nearly a factor of two. This result should be particularly useful for testing models that have a strong marginal-stability character, which typically find that the edge Ti is an important factor in controlling central Ti. Publication: This shot is unpublished. The physics of carbon blooms is described in Nuclear Fusion 31 (1991) p. 1811 by A. T. Ramsey. Other Info: