Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate
博士 === 國立成功大學 === 機械工程研究所 === 83 === Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate is presented now. The present investigation includes: (1)The prediction of the heat transfer rate between two na...
Main Authors: | , |
---|---|
Other Authors: | |
Format: | Others |
Language: | zh-TW |
Published: |
1995
|
Online Access: | http://ndltd.ncl.edu.tw/handle/44769978733236526436 |
id |
ndltd-TW-083NCKU0489092 |
---|---|
record_format |
oai_dc |
spelling |
ndltd-TW-083NCKU04890922015-10-13T12:53:36Z http://ndltd.ncl.edu.tw/handle/44769978733236526436 Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate 垂直平板兩側之不同熱傳系統的熱交互傳遞分析 Shiuh-Ming Chang 張旭銘 博士 國立成功大學 機械工程研究所 83 Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate is presented now. The present investigation includes: (1)The prediction of the heat transfer rate between two natural convection systems at different temperatures. (2)The prediction of the heat transfer rate between laminar film condensation of a saturated vapor and natural convection. (3)The prediction of the heat transfer rate between laminar film condensation of a saturated vapor and forced convection. (4)The prediction of the heat transfer rate between laminar film condensation of a saturated vapor and turbulent mixed convection. (5)The prediction of the heat transfer rate between laminar film condensation in the presence of a noncondensable gas and natural convection. But, in previous similar papers, the value of the cold fluid Prandtl number was assumed to approach infinite, so the effect of Prandtl number was neglected. The numerical results show that : (1)The present results calculated by one dimensional heat conduction model are in good agreements with experimental results.(2)In some conditions, the effect of the cold fluid Prandtl number could not be negligible. (3)As Ja<1, Nusselt- Rohsenow film condensation model is suitable. On the other hand, when Ja>1 (liquid FC-70R, Ja=3), the numerical solutions calculated by Nusselt-Rohsenow model are lower than the experimental results. (4)For Chapter 3 and 4,increasing Reynolds number Rec can decrease the wall temperature. (5)The presence of a very small amount of a noncondensable gas in the bulk of the vapor could cause a large buildup of the noncondensable gas at the liquid-vapor interface, so the temperature at the interface would decrease. It is worth memtioning that the interface temperature is not equal to wall temperature. Han-Taw Chen 陳寒濤 1995 學位論文 ; thesis 175 zh-TW |
collection |
NDLTD |
language |
zh-TW |
format |
Others
|
sources |
NDLTD |
description |
博士 === 國立成功大學 === 機械工程研究所 === 83 === Analysis for thermal interaction of two different heat transfer
systems on both sides of a vertical plate is presented now.
The present investigation includes: (1)The prediction of the
heat transfer rate between two natural convection systems at
different temperatures. (2)The prediction of the heat transfer
rate between laminar film condensation of a saturated vapor and
natural convection. (3)The prediction of the heat transfer
rate between laminar film condensation of a saturated vapor and
forced convection. (4)The prediction of the heat transfer rate
between laminar film condensation of a saturated vapor and
turbulent mixed convection. (5)The prediction of the heat
transfer rate between laminar film condensation in the presence
of a noncondensable gas and natural convection. But, in
previous similar papers, the value of the cold fluid Prandtl
number was assumed to approach infinite, so the effect of
Prandtl number was neglected. The numerical results show that
: (1)The present results calculated by one dimensional heat
conduction model are in good agreements with experimental
results.(2)In some conditions, the effect of the cold fluid
Prandtl number could not be negligible. (3)As Ja<1, Nusselt-
Rohsenow film condensation model is suitable. On the other
hand, when Ja>1 (liquid FC-70R, Ja=3), the numerical solutions
calculated by Nusselt-Rohsenow model are lower than the
experimental results. (4)For Chapter 3 and 4,increasing
Reynolds number Rec can decrease the wall temperature. (5)The
presence of a very small amount of a noncondensable gas in the
bulk of the vapor could cause a large buildup of the
noncondensable gas at the liquid-vapor interface, so the
temperature at the interface would decrease. It is worth
memtioning that the interface temperature is not equal to wall
temperature.
|
author2 |
Han-Taw Chen |
author_facet |
Han-Taw Chen Shiuh-Ming Chang 張旭銘 |
author |
Shiuh-Ming Chang 張旭銘 |
spellingShingle |
Shiuh-Ming Chang 張旭銘 Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate |
author_sort |
Shiuh-Ming Chang |
title |
Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate |
title_short |
Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate |
title_full |
Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate |
title_fullStr |
Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate |
title_full_unstemmed |
Analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate |
title_sort |
analysis for thermal interaction of two different heat transfer systems on both sides of a vertical plate |
publishDate |
1995 |
url |
http://ndltd.ncl.edu.tw/handle/44769978733236526436 |
work_keys_str_mv |
AT shiuhmingchang analysisforthermalinteractionoftwodifferentheattransfersystemsonbothsidesofaverticalplate AT zhāngxùmíng analysisforthermalinteractionoftwodifferentheattransfersystemsonbothsidesofaverticalplate AT shiuhmingchang chuízhípíngbǎnliǎngcèzhībùtóngrèchuánxìtǒngderèjiāohùchuándìfēnxī AT zhāngxùmíng chuízhípíngbǎnliǎngcèzhībùtóngrèchuánxìtǒngderèjiāohùchuándìfēnxī |
_version_ |
1716868417037795328 |