The two-dimensional steady and time-dependent fluid flow and heat transfer through periodic, wavy channels is numerically studied, for a fluid with a Prandtl number of 0.7, by means of an unstructured covolume method. The two geometrical configurations considered, a sinusoidal channel and an arc-sha
Numerical analysis of heat transfer and fluid flow in a three-dimensional wavy-fin and tube heat exchanger
β Scribed by Jiin-Yuh Jang; Li-Kwen Chen
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 812 KB
- Volume
- 40
- Category
- Article
- ISSN
- 0017-9310
No coin nor oath required. For personal study only.
β¦ Synopsis
The effects of different geometrical parameters, including tube row numbers (14 rows), wavy angles (0 = 8.95", 17.05", 32.21") and wavy heights (S = 0.751, 1.500 and 3.003 mm) are investigated in detail for the Reynolds number ReH (based on the fin spacing and the frontal velocity) ranging from 400 to 1200. Numerical results indicate that the row effect is less important in a wavy-fin as compared to plainfin counterpart. It is also found that, for equal wavy height, both the average Nusselt number and pressure coefficient are increased as the wavy angle is increased ; while for equal wavy angle, they are decreased as the wavy height is increased. The combination of (0 = 8.95", S = 1.500 mm) gives the highest flow area goodness factor (j/f). A comparison of the numerical results with the available experimental data is also presented.
π SIMILAR VOLUMES
Three-dimensional simulations of four louver-tube junction geometries are performed to investigate the effect on louver and tube friction and heat transfer characteristics. Three Reynolds numbers, 300, 600 and 1100, based on bulk velocity and louver pitch are calculated. Strong three-dimensionality
Measurements were made on the effects of circulating solid particles on the characteristics of fluid flow and heat transfer in the fluidized bed vertical shell and tube type heat exchanger with counterflow. The present work showed that the flow velocity range for collision of particles to the tube w
Principal heat transfer mechanisms in a fluidized bed have been classified into three categories, i.e. solid convection, gas convection and radiation. Among these mechanisms, the solid convection is a dominant mechanism in the bubbling fluidized bed. This solid convection is substantially caused by