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4 - Memorial University of Newfoundland DAI

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functional relationship relating these variables can be writlcn u:<br />

By the method <strong>of</strong> synthesis, the variables are cambilacd ih suela n way, so<br />

each ha. dimension d length. Therefore.<br />

0 ( T~~~,L~,~.,H.) =I). (4.6)<br />

Uaing L. b.i the repeating variable to non-dimensionalizc 1110 nlrovr cxprm.<br />

aion, the following expression results:<br />

(4.7)<br />

(4.8)<br />

After mpoundinr the above expression, tho lollowing cqantion is ohlai#ml:<br />

(4.9)<br />

The function @ may be oblained from a convcnionl wnvc llmry (c.g., Airy's<br />

small amplitude wave theory, Stokes' 3d or Llh ordcr wave Lhmriw, cle:.)<br />

depending on the application. For iinslancc,<br />

.<br />

if stnnll a~nplitadu wnvc!. ntc:<br />

king considered (the waveateepneas ia irrelcvn!~l),er~~nnlinv! (I.!)) rcxlom!r<br />

L.<br />

to:<br />

= (2) (4.10)<br />

For deep water and rmnll %mplitudo waves (since Ir. is no longcr rc!lcvnttt),<br />

the equation is furlher reduced to simply:

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