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Diffusion Reaction Interaction for a Pair of Spheres - ETD ...

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2<br />

D c = 0<br />

(5.1)<br />

∇ ext<br />

where D is the external Fickian diffusion coefficient and the concentration <strong>of</strong> the<br />

reactant is c. The concentration far from the two spheres is fixed as<br />

c ext = 0 , r 1 and ∞ → r 2 . (5.2)<br />

The remaining boundary conditions describe zeroth order generation <strong>of</strong> a<br />

substrate (reactant) occurring at the surface <strong>of</strong> sphere 2<br />

∂c<br />

∂r<br />

D ext<br />

2<br />

= −σ<br />

2 , 2 a2<br />

r = , (5.3)<br />

where it travels away from the source at a rate <strong>of</strong> D the substrate either escapes<br />

or is trapped and consumed inside sphere 1. The internal diffusion chemical<br />

reaction inside the sphere is described by<br />

D =<br />

2<br />

int∇<br />

cint<br />

kintcint<br />

, 1 1<br />

r ≤ a , (5.4)<br />

where D is the internal Fickian diffusion rate <strong>of</strong> the substrate with internal<br />

int<br />

concentration cint.<br />

The reactant is consumed inside sphere 1 by a first-order<br />

reaction with kinetic rate constant kint. The solution <strong>of</strong> equations (5.1) and (5.4)<br />

are both valid at the sink-medium interface because the reactant is transported<br />

106

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