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Boundary Lyer Theory

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216 X. Approximato n~ethods for steady eqllations d. Further examplcs 217<br />

well as in the shearing stress are concerned, and predict an earlier point of separation.<br />

W. Schocnauer found that thc separation angle is at$a = 1045Oas = 109TP'<br />

ol~t.ainat1 with t11c nit1 of the l'ohll~auscn approximation and $s = 108.8O suggested by<br />

tllc series cxp:ansion cont,inuctl up to the term z". A comparison between t,hc vclocity<br />

tli~t~ribut~ions, IGg. 10.8, leads to the conclusion t,l~at there cxist,s almost perfect<br />

agrwmrnt. hrf,wcrn t,Im exn.ct solut.ion and the npproxiniation in t.hc m.ngc of angles<br />

0 < 4 < !)On, t,lrat. is in t,l~c range of acc:clcrat,ctl c*xt.crnal flow. I 12 (K > O.O!IR), because the plot of X against A !.urns at, this poit~l<br />

(Table 10.2) and cantlot, tl~rmlore, be contirlucd 1)oyond K -- 0.0!15. Moreovor. for A > 12<br />

the vrloriby prnfilns l~rco~no r~nnrrcpt,al)le as t.liry rontnir~ point,^ for \vl~irl~ ti/II -.- I (Fig. 10.4).<br />

'I'l~rar cliffioid!.ira arc obviatcd wl~cr~ cqli. (10.37) is IIRC~.

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