I. Introduction
The rapid charging and discharging of electrical current on the magnet coils during the ITER Tokamak operation result in heat pulses which in turn induce pressure variation in the SHe cooling circuits where the pressure head for forced convection is generated by cold circulators. In particular, in the CS cooling circuit, the asymmetry of induced pressure rise at the suction and discharge of the circulator can result in pressure head values beyond the surge limit [1]. Such a phenomenon was not evident during the ITER CS model coil tests [2], mainly due to the fact that coils of different size (diameter) were wound layer by layer and connected in parallel. There the flow channels of the outer layers are less affected by the heat pulses than the inner ones and SHe flow across the circulator could persist. However, in case of the ITER CS system, all coils are wound pancake by pancake which dimensions are more or less identical (same flow channels in parallel) [3]. With such geometry the flow impedance of the inner layers will dominate throughout the whole pancakes during current shots and result in blocking of SHe flow across and trip of the circulator.