Transient heat transfer of superfluid 4He in nonhomogeneous geometries: Second sound, rarefaction, and thermal layer

被引:4
|
作者
Bao, Shiran [1 ,2 ]
Guo, Wei [1 ]
机构
[1] Natl High Magnet Field Lab, 1800 East Paul Dirac Dr, Tallahassee, FL 32310 USA
[2] Florida State Univ, FAMU FSU Coll Engn, Mech Engn Dept, Tallahassee, FL 32310 USA
基金
美国国家科学基金会;
关键词
2ND-SOUND SHOCK-WAVES; VORTEX-LINE DENSITY; LIQUID HELIUM-II; QUANTUM TURBULENCE; COUNTERFLOW TURBULENCE; MUTUAL FRICTION; PULSES; EVOLUTION; DYNAMICS; PROPAGATION;
D O I
10.1103/PhysRevB.103.134510
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Transient heat transfer in superfluid He-4 (He II) is a complex process that involves the interplay of the unique counterflow heat-transfer mode, the emission of second-sound waves, and the creation of quantized vortices. Many past researches focused on homogeneous heat transfer of He II in a uniform channel driven by a planar heater. In this paper, we report our systematic study of He II transient heat transfer in nonhomogeneous geometries that are pertinent to emergent applications. By solving the He II two-fluid equations of motion coupled with Vinen's equation for vortex-line density, we examine and compare the characteristics of transient heat transfer from planar, cylindrical, and spherical heaters in He II. Our results show that as the heater turns on, an outgoing second-sound pulse emerges, within which the vortex-line density grows rapidly. These vortices attenuate the second sound and result in a heated He II layer in front of the heater, i.e., the thermal layer. In the planar case where the vortices are created throughout the space, the second-sound pulse is continuously attenuated, leading to a thick thermal layer that diffusely spreads following the heat pulse. On the contrary, in the cylindrical and the spherical heater cases, vortices are created mainly in a thin thermal layer near the heater surface. As the heat pulse ends, a rarefaction tail develops following the second-sound pulse, in which the temperature drops. This rarefaction tail can promptly suppress the thermal layer and take away the deposited thermal energy. The effects of the heater size, heat flux, pulse duration, and temperature on the thermal-layer dynamics are discussed. We also show how the peak heat flux for the onset of boiling in He II can be studied in our model.
引用
收藏
页数:10
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