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pigmented colorants: dependence on media and time - Cornell ...

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∆i − =(K + S) idx<br />

202<br />

∆j − =(K + S) jdx (A.1)<br />

On the other h<strong>and</strong>, the gains in each flux come from scattering al<strong>on</strong>e. Assuming<br />

a single scattering event in the layer dx, the gains are:<br />

∆i + = Sj dx<br />

∆j + = Si dx (A.2)<br />

Then the total loss in each directi<strong>on</strong> is the loss minus the gain. Note that the<br />

upward-moving quantity is negated so that we can measure both changes in the<br />

same coordinate system.<br />

di =∆i − − ∆i +<br />

=(K + S) idx− Sj dx<br />

dj = − ∆j − − ∆j +<br />

=(K + S) jdx− Si dx (A.3)<br />

Letting the c<strong>on</strong>stant a = 1+ K<br />

<br />

yields the two differential equati<strong>on</strong>s:<br />

S<br />

di<br />

Sdx<br />

− dj<br />

Sdx<br />

= ai − j<br />

= aj − i (A.4)<br />

Adding these two equati<strong>on</strong>s together <strong>and</strong> rearranging the terms leads to:

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