22.01.2014 Views

Instantaneous Point-source Solution - IfH

Instantaneous Point-source Solution - IfH

Instantaneous Point-source Solution - IfH

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Section 3: Similarity solution to the one-dimensional diffusion equation 16<br />

To find C 1 we must use the conservation of mass:<br />

∫<br />

M = C(x, t)dV<br />

=<br />

= M<br />

which gives the constraint<br />

∫ ∞<br />

−∞<br />

V<br />

∫ ∞ ∫ a<br />

−∞ 0<br />

∫ ∞<br />

−∞<br />

C(η)2πrdr √ Dtdη<br />

f(η)dη<br />

(<br />

C 1 exp − η )<br />

dη = 1. (31)<br />

4<br />

To solve this integral we need to make one more change of variables<br />

to remove the 1/4 from the exponential. Thus, we introduce ζ such<br />

that<br />

ζ 2 = 1 4 η2 (32)<br />

2dζ = dη. (33)<br />

[PgUp] [PgDn] [Back]

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!