Even though the process of cryogenic chilldown is very complex, attempts are continuously being made to simulate the momentum and energy interactions accurately as in real case through CFD. One of the major reasons is the lack of reliable data and correlations that compass the parameters associated with cryogenic fluids. This work has taken the much needed first step in studying the effect of varying transfer line materials on their corresponding chilldown times. Chilldown in aluminium copper steel lines were investigated using validated computational fluid dynamics code (FLUENT 15.0). The time taken to completely chilldown o aluminiumis the fastest and requires minimum fluid mass compared to copper and steel . it is predicted through this computational technique that aluminium is the best material or chilldown as opposed to copper and steel Keywords: Cryogenics, Chill down, Two phase flow, Heat transfer rate
I. INTRODUCTIONCryogenic fluids have been used in various applications over the past century. One application that is continuously getting attention has been the use of cryogenic propellants for rocket propulsion. This interest is sparked by the fact that cryogenic propellants yield more energy and are more environmentally friendly, when compared to non-cryogenic propellants and the storage systems for these cryogenic propellants are lighter than those required for their non-cryogenic counterparts. The operation of a cryogenic propulsion system requires cooling of transfer line before establishing a steady flow of cryogenic fluid between various system components. The process of cooling down the equipment with cryogenic fluid is known as a cryogenic chilldown process. Cryogenic transfer line chill down is a transient heat transfer problem that involves rapid heat exchange from a solid structure to a fluid with phase change. It is necessary to know how long it takes to chill down a given transfer line for satisfactory operation. When liquid cryogen, for example nitrogen, at saturation temperature (77.6 K at 1 atm.) begins flowing through a tube initially at ambient temperature (300 K) the liquid instantly vaporizes near the tube wall. Thus a cross-section of the flow will have an outer vapour ring with a saturated liquid core. As the flow moves downstream, the liquid core evaporates and the vapour becomes superheated. As the tube wall cools, the liquid core penetrates further and further downstream. Eventually, the tube becomes filled with liquid. Reduction in fluid density by vaporization causes the average flow velocity to increase significantly. Prediction of chilldown time requires modelling of these transient phenomena and understanding of how they affect heat transfer from the tube wall to the flowing cryogen. Transient heat transfer processes between the liquid and transfer line cause vaporization of the liquid, and this phase change can cause transient pressure and flow surges in the liquid. As the transfer line is cooled, these effects diminish until the liquid reaches a steady flow condit...