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Boundary Lyer Theory

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568 XVIII. F~~ndamentnls of turbulent flow<br />

,I<br />

1 his is cxplnint\d 1)y the reqnir~mcnt~ of cont,inuity accortling to which, as we know,<br />

t,l~e r:~,l,c. ol' Ilow through any cross-scction ronains constant in time. The integral of<br />

1.11~ c:orrrl:~tion function It, that is, thc quai~t~ity<br />

IS I.llc sc:c.ol~tl vrloc.ilty, 11~' in eqm (14.1:1). is n~wsurcd at. tht: same 1ora.t.ion<br />

l)111 :II. a (~iIl'(w111, ~IIS~.:III~< of I,imn (71~' at, inst,ant tl and 11.; at instant t2 = tl -1- 0, we<br />

obtain the so-called autocorrelalion funcliott. The provision of spacc-t,imc corrcl t .1011s, '<br />

that is, of observations of two velocity components, oath measured at a tlilrrrrnt<br />

location in space and at a different instant in tirnc, allows us to gain a gootl tlr:tl<br />

of insight. As an example, we reproduce in Fig. 18.8 snch space-time corr~lnt~ions<br />

Dist.anco from wall:<br />

y/d = 0.24<br />

T5orrrtdary-layer t.hickncss:<br />

8 - 16.8 nini<br />

Fig. 18.8. Space-time correlations of velocity flnctuatio~~s in Lhr turlnrlcnt Iwu~ltlary lnynr on<br />

e flat plate, as measured by A. J. Favre, J. J . Caviglio nnd 11. .J. lhnns [tfi]<br />

ol)t.nincd by A. J. Favre and his coworkers (161 in tl~c Lnrl~ulcnt bountl:~ry Inyrr on<br />

a fl:l.t plata. 'l'l~e 1nrnpor:tl tlispl;~cctncl~~l,, t,,,, of t.hn m;tsimcr~~~ oI'(-:~(.ll (:Itrvv is inll)osc(I<br />

by 1.h~ passage of turbulent ctlrlics; tho odtlics move wit,ll nn a~~~~rosit~~;~l~c:<br />

vc*lotil.y<br />

which is equal t,o 0.8 U,. 'l'11e tlccrcasc in the maxima is thc rcsult of ;L procrss wl~ich<br />

can be visualized as follows: With the 1)assago of time, tho t,url)ulc~~l, ntltlirs losr t,l~cir<br />

intlividnality t,hrougll mixing with the surroutlding I,urbnlc~~t, flt~icl. Concurrc:nt,ly,<br />

ncw etltlics c:ont,inttously spring into being.<br />

An albrnativc tlcscript,ion of the st,nicturc of turbulcricc is obt,:~inctl wltc~~ a<br />

fr~q~~e,zcy analysis of the motion is provided instcad of a correlation fu~irt~ion. 'l'l~is<br />

leads 11s t,o the concrpt of the speclr.w~rr of a t.rrrl)~~lcnl, st,rc:~ni. f,ct I, clcnot.r thc -- Srcquency<br />

a.7~~tl F(n) (171, t.11~ fr:wtional con1,rnt of tlw root-t~~r:~~~-s(~~~ar(:<br />

v:~lur, IL'~, of<br />

t.11~ longil.utlinal Iluct,uat,ion wl~icl~ bclongs t.o 1 .l~ frcqucnvy ir~l~c~rvnl fro111 11, - t.o 11. I ,111.<br />

'I'IIO fnnct,ion F(n), which rcprcsent,~ - t,l~c tlcllsi1,y of 1.11~ tlislxil)r~l.io~~ ol' IL'VII ?I, is<br />

Icnown as t,l~c .spechd rlistrih~~tio,a of 71,'" l3y tlcfi~~itiorr, wr: must, I~avct

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