1997
DOI: 10.1007/s11665-997-0037-9
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Experimental determination of the first and second critical heat flux densities and quench process characterization

Abstract: The presence of "shock-film" boiling is seldom detected in most cooling curve quenchant characterization experiments and is often considered to be unimportant. In this paper, the experimental determination and calculation of the first critical heat flux density of shock-film boiling is described. The use of the first critical heat flux density to characterize the cooling behavior of various types of quenchant media and CVD surface coated metals is also described. Keywordsquench cooling stages, quench modeling,… Show more

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Cited by 48 publications
(6 citation statements)
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“…Film boiling should prevail during quenching with increasing bath temperature because critical heat flux density decreases with decreasing underheat  uh (see Eq. (8)) [9], [10]. The experimental results shown in Fig.…”
Section: Analysis Of Petrash's Experimentsmentioning
confidence: 99%
“…Film boiling should prevail during quenching with increasing bath temperature because critical heat flux density decreases with decreasing underheat  uh (see Eq. (8)) [9], [10]. The experimental results shown in Fig.…”
Section: Analysis Of Petrash's Experimentsmentioning
confidence: 99%
“…he author of the paper was dealing a long time with testing of different kinds of water salts solutions using spherical silver probe 20 mm in diameter. The silver probe was used to evaluate critical heat flux densities of water at different temperatures [1]. However, it was impossible to evaluate critical heat flux densities of water salt solution (electrolytes) using standard silver probe 20 mm in diameter because developed film boiling during quenching was completely absent.…”
Section: Introductionmentioning
confidence: 99%
“…The vapor film acts as a resistance to heat transfer towards the bulk of the subcooled liquid and affects the cooling rate history to the point of favoring the formation of unwanted microconstituents, thus reducing the mechanical properties of the material; (b) nucleate boiling, associated with high heating rates due to the formation of bubbles that remove large amounts of heat; and (c) pure convection (either natural or forced), i.e., without boiling, during which heat extraction diminishes towards zero. Additionally, in the quenching literature the occurrence of a socalled shock-boiling regime just before a stable vapor film forms has been reported (Kobasko et al, 1997); it usually occurs during the first 0.1 s after the heated probe is submerged in the quenching medium. Through experiments involving heating of metallic parts in a subcooled liquid, a transition zone, characterized by the coexistence of film boiling and nucleate boiling, has been identified (Nukiyama and Shiro, 1966;Shiro and Nukiyama, 1984).…”
Section: Introductionmentioning
confidence: 99%