Tokamak: TFTR Pulse Number: 43480 Contact: P. Efthimion Institution: PPPL, Princeton University Date of Shot: Oct 30, 1989 Analysis Code: TRANSP Run number: 43480a01 Analysis Date: August 20, 1997 Assumptions: Zeff profile assumed flat. This is an ohmic shot without beams to provide a CXRS measurement of Ti. Throughout the shot, Ti is calculated assuming chii = 15 x neoclassical, which is a representation that reproduces Ti in other ohmic shots in which the Ti profile was measured (see S. Scott et al., in Proceedings of the U.S.-Japan Workshop on Ion Temperature Gradient Driven Turbulent Transport, University of Texas at Austin, January 11-14, 1993, AIP conference proceedings 284). For technical reasons, the L-mode conditions in this scan were produced by helium gas puffing rather than by saturating the limiter with deuterium. The thermal plasma is a mixture of helium and deuterium. Absent a direct measurement of the helium density, the helium density profile was artificially set to be a fixed multiple of the electron density profile (nHe/ne = 0.325) to provide an appropriate ion dilution to approximately match the measured dd neutron emission. The electron temperature data for this shot represents an average of several similar shots and thus performs some averaging over sawtooth effects. Shot Desc.: This is the ohmic shot in a 4-shot L-mode temperature scan at constant density. Heating power ranges from ohmic to 13 MW. In the beam-heated shots NBI is injected from 3.5 to 4.5 seconds. The plasma reaches transport equilibrium in about 300 ms (at 3.8 seconds). At 4.0 seconds the plasmas were all perturbed by a small helium puff, which allowed the electron diffusivity to be measured through the time-dependent evolution of ne(r,t). Thus, this scan provides a comparison of the temperature dependence of chii, chie with De which are found to all increase with temperature as Te^(alpha) with alpha = 1.5-2.5. Publication: P. Efthimion et al., Phys. Rev. Lett. 66 (1991) p. 421. Other Info: These shots are identified as sequence LM1.