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Heat transfer wall

Assignee: Hitachi Cable Ltd
•
Filing: 1985-02-13
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Granted: 1986-08-19
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Expires: 2005-02-13
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Abstract

Abstract In a perforated heat conductive surface structure having voids under an outer surface and openings in the outer surface, in order to obtain a high performance in particular at a low pressure and low temperature region, there is provided a heat transfer wall in which a thickness of a wall at a ceiling of each void and a length of a passage of the respective openings are increased in predetermined ranges.

Inventors

  • 👤 Wataru Nakayama
  • 👤 Tadakatsu Nakajima
  • 👤 Heikichi Kuwahara
  • 👤 Akira Yasukawa
  • 👤 Takahiro Daikoku
  • 👤 Hiromichi Yoshida

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-11-09 14:45
CPC Classifications
F; F28; F28F; F28F13/00; F28F13/18; F28F13/185; F28F13/187

Claims Analysis

Total Claims: 2
Claim 1
Independent Claim 372 words
A heat transfer wall comprising a number of elongated voids formed in an outer layer of said heat transfer wall, upper lids forming a part of said heat transfer wall for partitioning said voids and an outer surface of said heat transfer wall, passages for communicating the respective voids and the outer surface of said heat transfer wall with each other, and restricted openings formed in said passages, said restricted openings having a cross-sectional area smaller than a maximum cross-sectional area of said voids and being independent of each other, and said heat transfer wall being made of a single kind of heat conductive material, wherein a thickness of said upper lids defined by a distance Z* (cm) between an upper end of each of said voids and the outer surface of said heat transfer wall and a length l (cm) of each of said passage extending from said voids to the outer surface of said heat transfer wall simultaneously meet the following condition in combination of the material of said heat transfer wall and a fluid flowing on said heat transfer wall: ##EQU7## where erf is the error function erf ##EQU8## is the thermal diffusivity of the heat transfer wall (cm 2 /sec); Ts is the saturation temperature of the boiling liquid (K); σ is the surface tension of the boiling liquid (dyn/cm); λ l is the thermal conductivity of the boiling liquid (W/kcm); θ v is the density of vapor of the vapor (g/cm 3 ); h fg is the evaporation latent heat of the boiling liquid (J/g); ν v is the dynamic viscosity coefficient of the vapor (cm 2 /sec); d o is the diameter of the restricted openings (cm); q w is the heat flux based on the projected area (W/cm 2 ); N A /A is the number density of bubbling points (N A /A=C b ·d o 0 .4 ·q w 0 .5 where C b =80 in case of Freon or liquefied nitrogen, and C b =95 in case of water); and C.sub.τ, C q , C f and C h are the constants determined by physical characteristics of the boiling liquid, where C.sub.τ ÷0.02, C q ÷0.0007, C f ÷0.1 and C h ÷0.06.
Claim 2
Dependent Claim 372 words
A heat transfer wall comprising a number of elongated voids formed in an outer layer of said heat transfer wall, upper lids forming a part of said heat transfer wall for partitioning said voids and an outer surface of said heat transfer wall, passages for communicating the respective voids and the outer surface of said heat transfer wall with each other, and restricted openings formed in said passages, said restricted openings having a cross-sectional area smaller than a maximum cross-sectional area of said voids and being independent of each other, and said heat transfer wall being made of a single kind of heat conductive material, wherein a thickness of said upper lids defined by a distance Z* (cm) between an upper end of each of said voids and the outer surface of said heat transfer wall and a length l (cm) of each of said passage extending from said voids to the outer surface of said heat transfer wall simultaneously meet the following condition in combination of the material of said heat transfer wall and a fluid flowing on said heat transfer wall: ##EQU7## where erf is the error function erf ##EQU8## is the thermal diffusivity of the heat transfer wall (cm 2 /sec); Ts is the saturation temperature of the boiling liquid (K); σ is the surface tension of the boiling liquid (dyn/cm); λ l is the thermal conductivity of the boiling liquid (W/kcm); θ v is the density of vapor of the vapor (g/cm 3 ); h fg is the evaporation latent heat of the boiling liquid (J/g); ν v is the dynamic viscosity coefficient of the vapor (cm 2 /sec); d o is the diameter of the restricted openings (cm); q w is the heat flux based on the projected area (W/cm 2 ); N A /A is the number density of bubbling points (N A /A=C b ·d o 0 .4 ·q w 0 .5 where C b =80 in case of Freon or liquefied nitrogen, and C b =95 in case of water); and C.sub.τ, C q , C f and C h are the constants determined by physical characteristics of the boiling liquid, where C.sub.τ ÷0.02, C q ÷0.0007, C f ÷0.1 and C h ÷0.06.

References Cited (Backward Citations)

US30077A Cited
US3566514A Cited
USRE30077E Cited
US4059147A Cited
US4168743A Cited
US4216826A Cited
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USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1989-08-18 1990-02-17 1990-08-19 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1993-08-18 1994-02-17 1994-08-19 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 1997-08-18 1998-02-17 1998-08-19 $7700.00 Window Closed / Lapsed

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