Kh. Finken et al., STUDIES ON BASIC PHENOMENA DURING THE PELLET INJECTION INTO HIGH-TEMPERATURE PLASMAS, Plasma physics and controlled fusion, 39(5A), 1997, pp. 351-360
The injection of hydrogen/deuterium pellets into a tokamak leads to a
sudden increase in the electron density, and subsequently to a profile
peaking of the density and an increase in the stored energy. Immediat
ely after the injection, different types of oscillations are excited.
On TEXTOR, the first type immediately follows the injection and the se
cond one is excited with a delay of more than IO ms. The oscillations
show a 'snake-like' structure and occur close to the q = 1 surface wit
h a frequency of 0.7-2 kHz. The radial location of the second oscillat
ion is slightly shifted with respect to the first one. A fast-cooling
phenomenon ('pre-cooling') in the core region of a plasma is often obs
erved at pellet ablation phase. A study on the relation between the 'p
re-cooling' and sawtooth oscillations suggests that the central value
of safety factor of plasmas, q(0), is kept sufficiently below unity ev
en just after the sawtooth crash. During pellet injection, the ablatio
n rate is strongly modulated; these modulations cause so-called 'stria
tions' in the ablation cloud. One model relates the striations to the
energy reservoir on the plasma flux surfaces and describes the possibi
lity of deriving the q-profile; the question of whether this method pr
ovides reliable results cannot yet be answered conclusively. The traje
ctory of the pellet in the plasma is in general not straight but defle
cted in the electron drift direction (OH discharges) or in the ion dri
ft direction (CO-NBI discharges). The cloud develops a helically struc
tured tail in the electron flow direction (toroidally) and in the elec
tron diamagnetic drift direction (poloidally). The tail structure is a
ttributed to charge-exchange processes and to plasma rotation.