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Maximum and Minimum Heat Flux and Temperature Fluctuation in Film-Boiling States in Superfluid Helium

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Advances in Cryogenic Engineering

Part of the book series: Advances in Cryogenic Engineering ((ACRE,volume 35 A))

Abstract

Superfluid liquid helium (helium-II), especially the subcooled helium-II, is said to have special advantages as a coolant of superconducting devices, particularly where there is a possibility of thermal hazard. First of all, helium-II has better cooling characteristics than boiling normal helium, that is, a large peak heat flux Q max [1,2] and also a large recovery heat flux Q min [3]. (At Q max, film boiling begins and at Q min, the liquid near the heated metal surface reenters the stable non-film-boiling.) For the stabilization of superconducting magnets, it is important that the mechanism of heat transfer to helium-II is understood. Investigations have been made into the behavior of transitions between the non-film-boiling state and the film-boiling state at critical heat fluxes (Q max, Q min) both in the saturated and in the subcooled helium-II, as well as the cooling stability in the film-boiling state. The mechanism of noisy film boiling which emits an audible high-frequency sound in the saturated helium-II [4], also was studied. So far, several investigators have observed the noisy film-boiling process by means of high-speed motion picture techniques and microphone techniques [6]. In the present research, the frequency of the temperature change was measured with the help of a microthermometer and a clear correlation was determined between the cooling condition and the temperature fluctuation of the metal surface.

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Abbreviations

d :

= channel height

f :

= requency of temperature fluctuation

H :

= immersion depth

Q :

= heat flux density per unit heated surface area

Q >max :

= maximum non-fihn-boiling heat flux (peak heat flux)

Q min :

= minimum film-boiling heat flux (recovery heat flux)

Q smin :

= recovery heat flux from silent film boiling

Q nmin :

= recovery heat flux from noisy film boiling

T :

= temperature of heated element surface

Tb :

= bath temperature

Δ T :

= T — T b

References

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Kobayashi, H., Yasukōchi, K. (1980). Maximum and Minimum Heat Flux and Temperature Fluctuation in Film-Boiling States in Superfluid Helium. In: Timmerhaus, K.D., Snyder, H.A. (eds) Advances in Cryogenic Engineering. Advances in Cryogenic Engineering, vol 35 A. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-9856-1_44

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  • DOI: https://doi.org/10.1007/978-1-4613-9856-1_44

  • Publisher Name: Springer, Boston, MA

  • Print ISBN: 978-1-4613-9858-5

  • Online ISBN: 978-1-4613-9856-1

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