4.7 Article

Experimental study on sodium Screen-Wick heat pipe capillary limit

Journal

APPLIED THERMAL ENGINEERING
Volume 227, Issue -, Pages -

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.applthermaleng.2023.120397

Keywords

Sodium heat pipes; Screens -wicks; Capillary pressure; Capillary limit; Dryout oscillations

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This study experimentally investigates the capillary limit of liquid metal wick heat pipes, exploring the transient temperature variations and physical mechanisms under high heat fluxes, frozen startup, and various inclination angles. The experiments reveal that the capillary limit leads to a rapid temperature increase of about 5 degrees C/s at the evaporator end, while the condenser and adiabatic section temperatures decrease. Dryout oscillations were observed with positive inclinations before reaching the capillary limit. After the capillary limit, reducing the power just below the limit does not result in heat pipe recovery, but reducing the power by about 30% of the critical heat flux is necessary.
Heat pipes continuously transport the latent heat of vaporization from the evaporator to the condenser in the heat pipes due to the capillary pressure created by the menisci in the wick pumping the condensed fluid back to the evaporator. The heat pipe heat transfer capacity is then limited by the capillary limit. However, fewer capillary limit experiments were conducted to investigate the transient temperature variations and physical mechanism at the capillary limit for liquid metal wick heat pipes. This work presents capillary limit transient measurements on a sodium screen-wick heat pipe for high heat fluxes, high heating rates during frozen startup, and negative and positive inclination angles. It also investigates the special behavior before and after dryout, including dryout oscillations and the recovery process to understand the cause and physical mechanism at the capillary limit. The direct cause of the capillary limit is that the evaporation rate exceeds the capillary-driven liquid supply to the evaporator. The experiments show that the capillary limit creates a rapid temperature increase of about 5 degrees C/s at the evaporator end, while the condenser and adiabatic section temperatures decrease. Dryout oscillations were observed with positive inclinations before the capillary limit. After the capillary limit, reducing the power to just below the limit does not lead to heat pipe recovery, but the power needs to be reduced by about 30% of the critical heat flux to make the heat pipe return to its normal operating state.

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