Temperatures, densities and confinement of deuterium plasmas confined
in tokamaks have been achieved within the last decade that are approac
hing those required for a D-T reactor. As a result, the unique phenome
na present in a D-T reactor plasma (D-T plasma confinement, a confinem
ent, a heating and possible alpha-driven instabilities) can now be stu
died in the laboratory. Recent experiments on the Tokamak Fusion Test
Reactor (TFTR) have been the first magnetic fusion experiments to stud
y plasmas with reactor fuel concentrations of tritium. The injection o
f about 20 MW of tritium and 14 MW of deuterium neutral beams into the
TFTR produced a plasma with a T-to-D density ratio of about 1 and yie
lding a maximum fusion power of about 9.2 MW. The fusion power density
in the core of the plasma was about 1.8 MW m(-3), approximating that
expected in a D-T fusion reactor. A TFTR plasma with a T-to-D density
ratio of about 1 was found to have about 20% higher energy confinement
time than a comparable D plasma, indicating a confinement scaling wit
h average ion mass A tau(E) proportional to A(0.6). The core ion tempe
rature increased from 30 to 37 keV owing to a 35% improvement of ion t
hermal conductivity. Using the electron thermal conductivity from a co
mparable deuterium plasma, about 50% of the electron temperature incre
ase from 9 to 10.6 keV can be attributed to electron heating by the al
pha particles. The approximately 5% loss of alpha particles, as observ
ed on detectors near the bottom edge of the plasma, was consistent wit
h classical first orbit loss without anomalous effects. Initial measur
ements have been made of the confined high energy alpha particles and
the resultant alpha ash density. At fusion power levels of 7.5 MW, flu
ctuations at the toroidal Alfven eigen-mode frequency were observed by
the fluctuation diagnostics. However, no additional a loss due to the
fluctuations was observed. These D-T experiments will continue over a
broader range of parameters and higher power levels.