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

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QWASI Multi-segment Equations<br />

I(i) is total input (mol/h) to each reach from emissions, the atmosphere, and any<br />

tributaries. It does not include advective inputs from other reaches.<br />

DT(i) is the sum of D values for losses by reaction, burial, and volatilization plus all<br />

advective losses from water, including net loss to sediment. The (i) refers to reach 1, 2,<br />

3, or 4.<br />

D(i,j) is water and particle flow between reaches i and j.<br />

J(i) is a D value for the net output from each reach.<br />

J(1) = DT(1)<br />

J(2) = DT(2) – D(2,1) D(1,2)/J(1)<br />

J(3) = DT(3) – D(3,2) D(2,3)/J(2)<br />

J(4) = DT(4) – D(4,3) D(3,4)/J(3)<br />

X(i) is the ratio of D values and is the fraction of the chemical in water and particle flow<br />

that enters downstream reach (reach 1 is upstream of reaches 2, 3, and 4).<br />

X(1) = D(1,2)/J(1)<br />

X(2) = D(2,3)/J(2)<br />

X(3) = D(3,4)/J(3)<br />

Fraction of total input received by each reach, including upstream reaches.<br />

Q(1) = I(1)<br />

Q(2) = I(2) + I(1) X(1) = I(2) + Q(1) X(1)<br />

Q(3) = I(3) + I(2) X(2) + I(1) X(1) X(2) = I(3) + Q(2) X(2)<br />

Q(4) = I(4) + I(3) X(3) + I(2) X(2) X(3) + I(1) X(1) X(2) X(3) = I(4) + Q(3) X(3)<br />

The solution for water fugacities fW(i) for each reach is as follows:<br />

fW(4) = {Q(4) + [fW(5) D(5,4)]}/J(4)<br />

fW(3) = {Q(3) + [fW(4) D(4,3)]}/J(3)<br />

fW(2) = {Q(4) + [fW(3) D(3,2)]}/J(2)<br />

fW(1) = {Q(4) + [fW(2) D(2,1)]}/J(1)<br />

The sediment fugacities fS(i) can then be calculated from the steady-state equation in<br />

Fig. 8.5.<br />

fs(i) = fw(i)(DD(i) + DT(i))/(DB(i) + DS(i) + DR(i) + DT(i)) with D values specific to each<br />

segment.<br />

Figure 8.8 Steady-state mass balance equations for a series of four QWASI models with<br />

flows in both directions.<br />

X, is a ratio of D values, namely the ratio of the box-to-box advective transfer D<br />

value and the total loss D value from the source. The denominators, J, contain terms<br />

for losses from each box, again modified by fractions undergoing box-to-box transfer.<br />

Inspection of the equations reveals the significance of each term. When the<br />

connections are more complex with branching, the equations must be modified<br />

©2001 CRC Press LLC

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