The effects of changing beam and plasma species on the edge transport barri
er are investigated for ELM-free hot ion H mode discharges from the recent
DT experiments on JET. The measured pressure at the top of the pedestal is
higher for mixed deuterium and tritium and pure tritium plasmas over and ab
ove the level measured in pure deuterium plasmas at the same heating power.
The pedestal pressure increases with beam tritium concentration for mixed
deuterium-tritium beam injection into deuterium plasmas where the measured
edge tritium concentration remains low. Alpha heating plays a significant r
ole in the core of such plasmas, and the possible impact on the edge is dis
cussed together with possible direct isotopic effects. Heuristic models for
the transport barrier width are proposed, and used to explore a wider rang
e of edge measurements including full power DD and DT pulses. This analysis
supports the plasma current and mass dependence for a barrier width set by
the orbit loss of either thermal or fast ions, though it does not unambigu
ously distinguish between them. The fast ion hypothesis could well account
for some of the JET observations, though more theoretical work and direct e
xperimental measurement would be required to confirm this. An ad hoc model
for the power loss through the separatrix, P(loss)proportional-to-n(edge)(2
)Z(eff,edge)I(p)(-1), is proposed based on neoclassical theory, a balloonin
g limit to the edge gradient and a barrier width set by the poloidal ion gy
roradius. Such a model is compared with experimental data from JET. In part
icular, the model ascribes the systematic difference in loss power between
the Mark I and Mark II diverters to the change in the measured Z(eff). This
change in Z(eff) is consistent with the observed change in impurity produc
tion, which is described in some detail, together with a possible explanati
on provided by the temperature dependence of chemical sputtering.