The multi-tubular reactor takes the form of a shell and tube heat exchanger. The baffles that became of interest were the disk and doughnut baffles as they provided a 15 % greater effectiveness than the commonly used segmental baffle. The shell side heat transfer coefficient is usually predicted by correlations developed by Donohue (1949) and Goyal & Gupta (1984) for disk and doughnut baffles. However, these correlations result in inaccuracies due to the complexity of the configuration. Therefore, Slipcevic (1978), had developed a new method to calculate the shell side heat transfer coefficient. The Slipcevic method takes into consideration the annular flow, the crossflow and the doughnut flow. However, certain portions were gone unconsidered by this method. Therefore, the aim of this study was to modify the Slipcevic method to generate a more accurate shell side heat transfer coefficient. The heat transfer coefficient calculated using the original Slipcevic method was determined to be 58.6 W/m^2. K. The modified method resulted in a coefficient of 49.9 W/m^2. K. The modification resulted in a coefficient 14.8 % less than the original method. Since the simulated value for the propylene process was 15.8 % lower than the Slipcevic procedure, this revealed that the modification was slightly more accurate. The difference of 6.5 % between the two percent differences may be due to inaccuracies resulting from the assumptions of triangular gaps and that the wall viscosities were equivalent to the bulk viscosities.
Read full abstract