TY - JOUR
T1 - Convective Heat Transfer Enhancement
T2 - Mechanisms, Techniques, and Performance Evaluation
AU - He, Ya Ling
AU - Tao, Wen Quan
N1 - Publisher Copyright:
© 2014 Elsevier Inc.
PY - 2014
Y1 - 2014
N2 - In this chapter, the existing mechanisms for enhancing single-phase convective heat transfer are reviewed and the fundamental mechanism, that is, to reduce the intersection angle between fluid velocity and temperature gradient, is presented in detail. This basic idea is called the field synergy principle (FSP). A great number of examples are provided to demonstrate the validity of the FSP. Some typical convective heat transfer phenomena are analyzed and found that their characteristics can be well understood by the FSP. An effective way for improving convective heat transfer performance of an existing heat transfer structure is to reveal the locations with a bad synergy (i.e., large local synergy angle) and improve the performance by changing the local structure of the surface. Examples of new enhanced surfaces are provided which are developed under the guidance of the FSP. It is demonstrated that for the best synergy case where fluid velocity coincides with temperature gradient, the exponent in Nu∞Rem reaches its maximum value of 1. Then, the thermohydraulic performance comparisons of the enhanced configurations with the reference one are discussed under three constraints: identical pumping power, identical pressure drop, and identical flow rate. All the three constraints can be unified in a picture with log(fe/fo) and log(Nue/Nu0) as abscissa and ordinate, respectively. The entire plane is divided into four quadrants by the two coordinates, and the first quadrant is the most frequently encountered. An enhanced technique can be represented in this plot and the constraint under which heat transfer is enhanced can be clearly identified.
AB - In this chapter, the existing mechanisms for enhancing single-phase convective heat transfer are reviewed and the fundamental mechanism, that is, to reduce the intersection angle between fluid velocity and temperature gradient, is presented in detail. This basic idea is called the field synergy principle (FSP). A great number of examples are provided to demonstrate the validity of the FSP. Some typical convective heat transfer phenomena are analyzed and found that their characteristics can be well understood by the FSP. An effective way for improving convective heat transfer performance of an existing heat transfer structure is to reveal the locations with a bad synergy (i.e., large local synergy angle) and improve the performance by changing the local structure of the surface. Examples of new enhanced surfaces are provided which are developed under the guidance of the FSP. It is demonstrated that for the best synergy case where fluid velocity coincides with temperature gradient, the exponent in Nu∞Rem reaches its maximum value of 1. Then, the thermohydraulic performance comparisons of the enhanced configurations with the reference one are discussed under three constraints: identical pumping power, identical pressure drop, and identical flow rate. All the three constraints can be unified in a picture with log(fe/fo) and log(Nue/Nu0) as abscissa and ordinate, respectively. The entire plane is divided into four quadrants by the two coordinates, and the first quadrant is the most frequently encountered. An enhanced technique can be represented in this plot and the constraint under which heat transfer is enhanced can be clearly identified.
KW - Convective heat transfer
KW - Enhancement of heat transfer
KW - Field synergy principle
KW - Performance comparison plot
KW - Single-phase flow
KW - Thermohydraulic performance
KW - Waste heat recovery
UR - https://www.scopus.com/pages/publications/84919497510
U2 - 10.1016/bs.aiht.2014.09.001
DO - 10.1016/bs.aiht.2014.09.001
M3 - 文章
AN - SCOPUS:84919497510
SN - 0065-2717
VL - 46
SP - 87
EP - 186
JO - Advances in Heat Transfer
JF - Advances in Heat Transfer
ER -