18.06.2013 Views

Boundary Lyer Theory

Boundary Lyer Theory

Boundary Lyer Theory

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

518 XVI I. Origin of turhr~lcncc 11 c. Effects duc to heat transfer and cornprcsnihilil.y 510<br />

rtl 11y n~lrncrirnl rnlrulnt,ions thnt with n region in tho boundary layer whcrc lk > 1<br />

tI1rr.c- nrc- :In inlinitc nrlmbcr of nculml wnvc numbers, or modes, with the sarnc plrasc<br />

vrlocity c,. 'l'hr mult,iplc modes arc n result. of the change in the govcrning tlilPcrc:nt.inl<br />

rquation for, say, thc: ~mwurc oscillntictn from rlliptic whon MZ < 1 to hyperbolic<br />

\vhrn M" I. 'l'l~e first motlo is t.lx snmn as in incomprrssiblc flow, nntl was first<br />

rotnl~~trtl I'IW c~otnpr(~ssil~lc flow 1)y Ir. IATS tu10 1':. Itc:sllot.ko 11421. Thc ntltlit.ionn1,<br />

or I~ighrr. rnotlw hnvo no incornprc~ssil~lc ronnt,crpxrts. c, = c,, MZ, first, reaches<br />

11nit.y at M, 2.2, nntl the uppcr I~ountlary of t,hc rcgion of supersonic relative flow<br />

is nt ?I/(> -- 0.16, 0.43, 0.50, Lor f& =- 3, 5, 10, rcsprctivcly.<br />

..<br />

lhc multiple 11tmt.rn1 di~t~url~nnrcs wit,lr phnsc vdocit,y c8 are not tho only ones<br />

possiblo wllcw ME, > 1. Thcrc nrr also rnult.iplc ncut,rnl dist,urbances wit.h U, < c,<br />

< Il, -t a,. Tllrse dist,nrbnnccs (lo not. tlcpond on the boundary layer having a<br />

gc.nrrnlizcd inllrxion point,. I~urt.llcrmore, there nre always adjacent amplified tlist~rlrlmnrrs<br />

of t IIC .w~rre t?/pr idh, plrass 11e1ocitie.s c, < I/,. Co~tacquentl?/, the co~rr.prossil)le<br />

Ooi~?tdar?/ /fl?/rr is isnslable lo frictioltkss dislicrba~~ces rrgardloss of any other f~aturen o/<br />

thc idoci/?/ rr~rtl hrg~cr(r/rtrr profilrs (1,s lonq n.p th,rre in a rqlion idtrre M2 > 1.<br />

A limiting fn.rt,or in t,he amplifim.t,im of first,-motln tlisturbnnccs is t.hnt c, must<br />

lir I)c:t.wcvw ro n.11tl r,. Any lhing t,llnb incrcnsrs the diffcrrnoo cr - co nlso incrc-asps thc<br />

nmpIilic:nt~ion f:~.c:Ior /?,. As shown Iiy Iqig. 17.24, t,llis tlifkroncc can be cl11it.c stnnll.<br />

Tho co~lst.rn.int inlposrtl I)y co, which tlnlilrc c, is nnrclnkcl to the boundary-layer<br />

profile, call only 1)o rrnlovctl 11y consirlcring n moro general form of disturbancc than<br />

has I)crn usrtl up to t.llis point,. With<br />

As n rcsult of c, - co increasing wit,ll {I t.ho ~naxirrlr~tn nmpliBcnt,ion fnet,or of<br />

t

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

Saved successfully!

Ooh no, something went wrong!