We studied heat transfer between copper tube and two-phase helium for
different flow patterns. We can reach stratified wavy, intermittent an
d dispersed flow. The copper cell have two temperature sensors placed
on top and bottom of the tube. For all flow regimes the upper and lowe
r sensors record different heating in spite of the copper high thermal
conductivity. The temperature ratio between upper and lower sensors c
an be up to 20. This difference vanishes for dispersed flow. Moreover,
for both intermittent and stratified wavy flow, the boiling crisis oc
curs for heat flux of about 2 000 Wm(-2) and for the whole section. As
expected no boiling crisis appears for dispersed flow.