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

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1<br />

∫<br />

− 1<br />

2δ<br />

nm<br />

Pn<br />

( z)<br />

Pm<br />

( z)<br />

dz = , (B.32)<br />

1+<br />

2n<br />

Integrating the first term is done by considering two separate cases,<br />

• when j = 2 n + 1,<br />

n = 0,<br />

1,<br />

2,...<br />

, is odd and m = 2k<br />

, k = 0,<br />

1,<br />

2,...<br />

, is even<br />

(the m sum begins at j + 1,<br />

or. 2 n + 2 and the i sum goes from P to<br />

P1<br />

),<br />

• and when j = 2n<br />

, n = 0,<br />

1,<br />

2,...<br />

, is even and m = 2 k + 1,<br />

k = 0,<br />

1,<br />

2,...<br />

, is odd<br />

(the m sum begins at 2 n + 1,<br />

and the i sum goes from up to P ).<br />

Pm −1<br />

0<br />

Finally the last term is directly integrated using the orthogonality condition <strong>of</strong><br />

Legendre polynomials. After some rearranging the resulting reaction rate <strong>of</strong> the<br />

diffusion-limited sphere 1 ( c 0 ) in the presence <strong>of</strong> sphere 2 is<br />

1 =<br />

⎛<br />

⎜<br />

⎜<br />

= ⎜ +<br />

( )×<br />

⎜ ∑<br />

⎜<br />

⎜<br />

⎝<br />

∞<br />

1<br />

R 1 1 sinh μ1 W j μ1<br />

2<br />

j=<br />

0<br />

⎧<br />

⎪<br />

⎨<br />

⎪<br />

⎪<br />

⎩<br />

⎡<br />

( μ1)<br />

cosh⎢<br />

1<br />

⎣<br />

⎡<br />

sinh⎢<br />

⎣<br />

( μ + μ )<br />

( μ + μ )<br />

1<br />

( c − c )<br />

⎛ 1 ⎞⎤<br />

2<br />

⎜ j + ⎟⎥<br />

+<br />

⎝ 2 ⎠⎦<br />

c<br />

⎛ 1 ⎞⎤<br />

2 ⎜ j + ⎟⎥<br />

⎝ 2 ⎠⎦<br />

W j<br />

2<br />

0<br />

j<br />

0<br />

152<br />

⎫<br />

W ( μ 2 ) ⎪<br />

⎬<br />

⎪<br />

⎪<br />

⎭<br />

⎞<br />

⎟<br />

⎟<br />

⎟ ,<br />

⎟<br />

⎟<br />

⎟<br />

⎠<br />

m−1<br />

(B.33)

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