Page 46 - Adsorbents fundamentals and applications
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TEMPERATURE SWING ADSORPTION AND PRESSURE SWING ADSORPTION  31

            concentration and flow rate from a PSA process, without the use of surge or
            mixing tanks, vary with time. Product recovery measures the amount of com-
            ponent that is contained in the product stream divided by the amount of the
            same component in the feed mixture. Adsorbent productivity is measured by the
            amount of product or feed mixture processed per unit amount of sorbent per
            unit time. For a given separation, the product purity is predetermined, the energy
            requirement is usually proportional to the recovery, and the size of the sorbent
            bed is inversely proportional to the sorbent productivity. It is important to bear in
            mind that these three parameters are interrelated for any given PSA process, and
            the interrelationship can be determined only through a model for the process. In
            addition to these parameters, the term “strong adsorptive” will be used to refer
            to the strongly adsorbable gas, whereas “weak adsorptive” will be used for the
            weakly adsorbable gas. The product that mostly contains the weak adsorptive
            may also be called “loosely light product” or “raffinate”, the latter is in analogy
            to liquid–liquid extraction.
              The basic PSA cycle was described by Skarstrom in 1960 (Skarstrom, 1960;
            1972). A similar cycle was the Guerin–Domine Cycle, invented at about the
            same time (Guerin–Domine, 1964; see a detailed account of these inventions
            in Yang, 1987). The latter was the basis for the modern vacuum swing cycle.
            The major additions to these cycles are co-current depressurization (CD) and
            pressure equalization (PE) steps. The CD step was added to increase product
            recovery, whereas the pressure equalization step was added to conserve the
            mechanical energy.


            Skarstrom Cycle. The Skarstrom cycle uses a two-bed apparatus as shown in
            Figure 3.1. There are two main cycle steps: high-pressure adsorption and low-
            pressure purge. In between these two steps are two pressure-changing steps. These
            cycle steps are illustrated in Figure 3.2. After the high-pressure adsorption step,
            the first bed is depressurized to atmospheric (or a low) pressure. At the same
            time the compressed feed mixture is switched to the second bed to repressurize
            it. It then starts the adsorption step at the feed pressure. A fraction of the purified
            effluent from the second bed is passed through the first bed, countercurrent to the
            feed direction, to purge the bed at atmospheric (or low) pressure. After the purge,
            the unit is ready for the next cycle. Thus each bed undergoes two half-cycles,
            the times of which are equal. For a purification process, steady and continuous
            flows of both feed and purified product are achieved.
              Two useful intuitive ideas were also described by Skarstrom’s invention. First,
            short cycles and low throughput per cycle should be maintained in order to “con-
            serve the heat of adsorption.” This idea was derived from the observation that
            long cycles and high throughputs would result in hot beds during adsorption
            and cold beds during regeneration, both detrimental to separation. The second
            idea was that the volume of both purge and feed, at their respective pressures,
            should be at least equal to ensure complete purge, or displacement, during regen-
            eration. These two basic ideas have been determined to be very useful in later
            developments.
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