Resin Overheating - h1015v2

Breakthrough and Exhaustion

Resin Overheating - h1015v2_81

Chemistry Volume 2 of 2
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R CH₂N(CH₃)₃OH R CH₂OH N(CH₃)₃ heat R CH₂N(CH₃)₃OH R CH₂N(CH₃)₂ CH₃OH heat DOE-HDBK-1015/2-93 DISSOLVED GASES, SUSPENDED SOLIDS, AND pH CONTROL Principles of Water Treatment CH-04 Rev. 0 Page 24 As solution passes through the resin column, the relative amounts of ammonium and hydrogen ions on the resin change. The actual exchange process occurs primarily in a relatively narrow band of the column rather than over the entire length. This band is called the exchange zone. Assuming the column is vertical and that solution flows from top to bottom, the resin above the exchange zone is depleted; that is, practically all the exchange capacity has been used. Below the exchange zone, essentially none of the resin's exchange capacity has been used. As more and more solution flows through the column, the exchange zone gradually moves downward as more of the resin is depleted. Eventually, as the exchange zone approaches the end of the column, small amounts of NH begin to appear in the effluent. The point at which this occurs is called 4 + breakthrough. If more solution passes through the resin, the concentration of NH in 4 + the effluent increases until it is the same as the concentration in the influent. This condition is called exhaustion and indicates that essentially all the exchange capacity of the resin has been used. (Because of the equilibrium nature of the exchange process, a small amount of the resin may remain in the hydrogen form, but not enough to remove any more ionic impurities.) Note that because the exchange zone in this case was narrow, a relatively small volume of solution takes the resin from breakthrough to exhaustion. Resin Overheating The potential for elevated temperatures exists during most conditions of facility operation, we will examine in detail the processes that occur if the resin in an ion exchanger is overheated. Although the inert polystyrene basic structure of resin is stable up to fairly high temperatures (approximately 300 F), the active exchange sites are not. The anion resin begins to decompose slowly at about 140 F, and the decomposition becomes rapid above 180 F. The cation resin is stable up to about 250 F. Because these temperatures are well below normal reactor coolant temperatures, the temperature of the coolant must be lowered before it passes through the ion exchange resin. The anion resin (hydroxyl form) decomposes by either of two mechanisms with approximately equal probability. (4-24) or (4-25)

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