THE RELATION (RATIO) BETWEEN THE AVERAGE AND MAXIMUM VELOCITIES DURING TURBULENT MOTION IN PIPES

Document Type: 
Collection: 
Document Number (FOIA) /ESDN (CREST): 
CIA-RDP82-00039R000100270010-1
Release Decision: 
RIPPUB
Original Classification: 
R
Document Page Count: 
3
Document Creation Date: 
December 22, 2016
Document Release Date: 
April 25, 2012
Sequence Number: 
10
Case Number: 
Publication Date: 
April 9, 1952
Content Type: 
REPORT
File: 
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PDF icon CIA-RDP82-00039R000100270010-1.pdf1.38 MB
Body: 
Declassified in Part -Sanitized Copy Approved for Release 2012/04/25 :CIA-RDP82-000398000100270010-1 13~twcacn. ~~he; ~.v'~xa?;a and l~f~~~imvm ........~~......_.r. Velcc~.~l,i~s l~urin~ ~]~ur~ulc;n,~~~ian in F~.pes ad Akadem.ii I~1a.ub~ S~SR, VOZL1l11G r19, 110 3, pp 115" ~ ol~l ~' ~'fiosca~~r~t~enin~rac?.c 21 July ti9~1, Declassified in Part -Sanitized Co A roved for Release 2012J04/25 :CIA-RDP82-000398000100270010-1 , PY pP rSTAT; :STAY. Declassified in Part -Sanitized Copy Approved for Release 2012/04/25 :CIA-RDP82-000398000100270010-1 "The ~~,elatian '(patio) between the Average and I,~axa.mum iti~es Dura.ng 'turbulent ~[ota.on in Pa.pee't Veloa ~,, D, Al t tshu~' Note: 'the following 'repoz~~ appeared in the re~u~~x ' section of the thrice-~nlonthly journal. Uok~.adY HydrarrGechanics a ~ ~ SSS~Z Volume: 79, No. 3 ' (21 July 1951), AkadE.rn~..a. Nauk , ~. 7:t had been subrna.tted by acadamic9.an A. I? pages ~~05 6> ?krasov, 31 day 1~1~1, til now there has been no theoretcttlly-based Up urr a for determining the dependence of the field coefficient formal tio. of average flo~rr velocity to the maximu~.), during tur- (ra ent rxtotion in smooth pipes, upon f~eynolds' number. Now bul this formula is obtained iri a perfectly elementary manner from prandtl's equation (1)~ (1) ~= V are res ectively the maximum, dynamical,... and (Umax, Uti, , p ocit -and D is Prandtl's constant), and from the av~,rage vel y, for the coefficient of frictian (2)~ formula in the following way Utilizing the familar relation U%~ place of (1), tine have Umax ~ ~ = 1 ~' (2) y $ in ,Substituting (2) into (3), after transformations we ~, .. ,~0 (~.o~ lg P,e--x..30 .? D) , (4) obtain V~Umax - (5.0~ lg e ~ , )~ ll :: ~ 0 accordirr~; to experiments of l~ikuradz~, Assuming }?3 ( ' D fluctuates from 3:$ to ~.6), we `haves the qudntlty ~, ?- ,.,y ~. _ ~, ~ ~f ~ ~~ ~,7i :b+~^t ,gyp; Y' The ..agreement of experience and theory in t'