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Boundary Lyer Theory

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418 XV. Non-slmrly l~orrnclnry Inyrr~<br />

I5 x a 111 1) 1 t- . Ci~c~tltrr r!/litctla~<br />

I'or tJto rircwlar cylintlcr of ratlitis 11 in n strcntn of vrlocity I/,, we obtth:<br />

as swtt from rrp. (15.45). 'l'llc tlist.nnco covrrctl uut,il sapration begins is R, = 1, I/,,<br />

st, t.Ir:~t,<br />

b. Bo~lnclnry-lnyrr forinntion nhrr inipnlnivc dart of niotio~~<br />

Inserting tho vnlucn from cqns. (15.47) intorrp. (I5.46), wr find that I.l~c tin~r cln11s~tl IIIII~I t,lie<br />

onset of ucpnrntion is<br />

I'ig. 15.2. I)int,:~nce 8<br />

t.ravrrsccl by rlliptic cylinelrr<br />

r~nt.il thc: onset elf<br />

scpnrntion in t.hc vnuo<br />

of i~npnlsivc? :~.ctdt.r:~t,ion<br />

fro111 red,<br />

4<br />

y, = 0 for Px < ---<br />

3 '<br />

For k = I cqn. (16.48) t,r~~nnfortn~ inlo cqn. (16.4f;) for 1110 cirex11:ir e:yIit~tlvr. Ibgit~t~i~~g with<br />

tlh vnlr~o the ti~nn L, for tho onsct of sc[)nrnl.ion clccrcn~as will1 i~~e:rc::tninl: k -7 h/w. IIII~I 1.11~.<br />

position of tho point of nepnrntion move8 Crom the end of &xis rx f,ow~lrtls LIic cntl of nxia b. 111<br />

the limit D/n -+ m, i.e. br a plate at right angles to tlw tlirrc~fion of motion, wc 11:tvr I ,<br />

and !I, - 11. Iirnce the onsct of srparation is i~n~nctlint*? for t.Itc c.:~st: of n fl:lt pl:lfn ~wrpc*ntlit.~~inT<br />

10 t.hr rlirrction of rnot,ioti, n.ntl it tnkes plrmc nt ths ctlgc.

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