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McKay, Donald. "Front matter" Multimedia Environmental Models ...

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containing nonequilibrium quantities of benzene to flow into and out of the tank at<br />

constant rates as shown in Figure 2.1B. But equilibrium and a steady-state condition<br />

are maintained, since the concentrations in the tank and in the outflows are at a<br />

ratio of 1:4. It is possible for near equilibrium to apply in the vessel, even when<br />

the inflow concentrations are not in equilibrium, if benzene transfer between air<br />

and water is very rapid. Figure 2.1B thus illustrates a flow, equilibrium, and steadystate<br />

conditions, whereas Figure 2.1A is a nonflow, equilibrium, and steady-state<br />

situation.<br />

In Figure 2.1C, there is a deficiency of benzene in the inflow water (or excess<br />

in the air) and, although in the time available some benzene transfers from air to<br />

water, there is insufficient time for equilibrium to be reached. Steady state applies,<br />

because all concentrations are constant with time. This is a flow, nonequilibrium,<br />

steady-state condition in which the continuous flow causes a constant displacement<br />

from equilibrium.<br />

In Figure 2.1D, the inflow water and/or air concentration or rates change with<br />

time, but there is sufficient time for the air and water to reach equilibrium in the<br />

vessel, thus equilibrium applies (the concentration ratio is always 4), but unsteadystate<br />

conditions prevail. Similar behavior could occur if the tank temperature changes<br />

with time. This represents a flow, equilibrium, and unsteady-state condition.<br />

Finally, in Figure 2.1E, the concentrations change with time, and they are not<br />

in equilibrium; thus, a flow, nonequilibrium, unsteady-state condition applies, which<br />

is obviously quite complex.<br />

The important point is that equilibrium and steady state are not synonymous;<br />

neither, either, or both can apply. Equilibrium implies that phases have concentrations<br />

(or temperatures or pressures) such that they experience no tendency for net transfer<br />

of mass. Steady state merely implies constancy with time. In the real environment,<br />

we observe a complex assembly of phases in which some are (approximately) in<br />

steady state, others in equilibrium, and still others in both steady state and equilibrium.<br />

By carefully determining which applies, we can greatly simplify the mathematics<br />

used to describe chemical fate in the environment.<br />

A couple of complications are worthy of note. Chemical reactions also tend to<br />

proceed to equilibrium but may be prevented from doing so by kinetic or activation<br />

considerations. An unlit candle seems to be in equilibrium with air, but in reality it<br />

is in a metastable equilibrium state. If lit, it proceeds toward a “burned” state. Thus,<br />

some reaction equilibria are not achieved easily, or not at all.<br />

Second, “steady state” depends on the time frame of interest. Blood circulation<br />

in a sleeping child is nearly in steady state; the flow rates are fairly constant, and<br />

no change is discernible over several hours. But, over a period of years, the child<br />

grows, and the circulation rate changes; thus, it is not a true steady state when<br />

viewed in the long term. The child is in a “pseudo” or “short-term” steady state.<br />

In many cases, it is useful to assume steady state to apply for short periods,<br />

knowing that it is not valid over long periods. Mathematically, a differential<br />

equation that truly describes the system is approximated by an algebraic equation<br />

by setting the differential or the d(contents)/dt term to zero. This can be justified<br />

by examining the relative magnitude of the input, output, and inventory change<br />

terms.<br />

©2001 CRC Press LLC

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