Performance of agitated gas-liquid contactors
Performance of agitated gas-liquid contactors
复制标题
DOI:
10.1021/ie50414a005
复制
发表时间:
1944-01-01
影响因子:
--
通讯作者:
Miller, SA
中科院分区:
文献类型:
--
作者:
Cooper, CM;Fernstrom, GA;Miller, SA
FOR absorption applications to which conventional plate or packed columns are not well suited, such as gas-liquid reac-tions involving more than two phases, agitated gas-liquid contactors are useful. Outside of a few laboratory studies of specific reactions carried on in agitated flasks, no investigations of mechanical gas dispersers have been reported, and no rational basis for the design of this important type of equipment exists. This paper describes a laboratory method of evaluating the variables. pertinent to such equipment and proposes a basis for the design of plant gas-liquid reactors. The rate of solution of a gas in a liquid is a function of the following factors: area of gas-liquid interface, temperature, time of contact, magnitude of driving force, and intensity of agitation. If simultaneous absorption (physical) and reaction (chemical) are occurring, such additional factors as solute or catalyst con-centration, pH, and light intensity may be involved. In a given system, these reaction factors and the itemsof temperature and driving force are usually either fixed or easily controllable to give the optimum conditions; area of contact, time of contact, and agitation thus become the variables most important to the design of gas-liquid contacting equipment. Strictly speaking, gas dispersers are concerned only with the variables of area and time of contact, since it is their function to divide the gas into bubbles and to disperse these bubblesthrough the liquid phase. In so doing, however, they always produce within the liquid phase a degree ofturbulence which may vary from that produced by the gas stream emanating from a sparger into an unagitated reactor, to that developed by a high-speed impeller operating in a baffled vessel. Liquid turbulence is in itself not undesirable, since most absorptions are controlled par-tially or entirely by the liquid-film resistance, and agitation of the liquid phase therefore enhances the rate of mass transfer. Also, eddy currents in the body of the liquid may improve con-tactor performance by directly increasing the liquid shear on the dispersed bubbles and by lengthening the average retention time of the bubbles. The most direct method, then, of evaluating disperser performance is by count and measure-ment of the bubbles pro-duced, obviously not a practical scheme. An indirect but more practi-cal procedure is to measure the rate of gas solution for some system in which the gas-film resistance entirely controls. Such meas-urement does not differentiate between area of contact and re-tention time, but it does largely eliminate the variable of agitation intensity. Unfortunately systemswhose resistance is pri-marily in the gas film are not susceptible to simple, dependable measurement; the easiest, most reliable, batch laboratory de-terminations of absorption rate must be made on systems in which the liquid-film resistance is considerable. Such a system pro-vides a third means of disperser evaluation which, although less desirable from the standpoint of developing fundamental knowl-edge, should be satisfactory when applied to commercial designs operating in systems with the usual high liquid-film resistance.