Skip to main content

NACA-RM-L7A24 · Two-Dimensional Wind-Tunnel Investigation of Modified NACA 65(sub 112)-111 Airfoil with 35-Percent-Chord Slotted Flap at Reynolds Numbers up to 25 Million

NASA (NTRS) · 1947

Open the PDFPublic domain · NASA (NTRS)Technical Reports

Overview

An investigation has been made in the Langley two-dimensional low-turbulence tunnels to develop the optimum configuration of a .035-chord slotted flap on an NACA 65(sub(112)-111 airfoil section modified by removing the trailing-edge cusp. Included in the investigation were measurements to determine…

Pages
·
19

Key points

  • The investigation focused on the optimum configuration of a 0.35-chord slotted flap on a modified NACA 65(112)-111 airfoil.
  • Tests were conducted in a low-turbulence wind tunnel at Reynolds numbers ranging from 3.0 x 10^6 to 25.0 x 10^6.
  • The optimum flap configuration at high Reynolds numbers was found to be a flap deflection of 35 degrees.
  • The maximum section lift coefficient increased from 2.15 to 2.11 as the Reynolds number increased from 9.0 x 10^6.
  • Shifts in the linear portion of the lift curve due to variations in Reynolds number were reduced by altering the flap position.
Frequently asked questions
What was the purpose of the investigation?

The investigation aimed to develop the optimum configuration of a 0.35-chord slotted flap on a modified NACA 65(112)-111 airfoil and to determine the dependence of this configuration on the Reynolds number.

What Reynolds numbers were tested in the study?

Tests were conducted at Reynolds numbers ranging from 3.0 x 10^6 to 25.0 x 10^6.

What was the optimum flap deflection found in the study?

The optimum flap configuration at high Reynolds numbers was determined to be a flap deflection of 35 degrees.

How did the maximum section lift coefficient change with Reynolds number?

The maximum section lift coefficient increased from 2.15 to 2.11 as the Reynolds number increased from 9.0 x 10^6.

How were shifts in the lift curve addressed?

Shifts in the linear portion of the lift curve caused by variations in Reynolds number were either eliminated or considerably reduced by altering the flap position.

Document

RESEARCH M€MORANDUM

NATIONAL ADVISORY COMMITTEE

FOR AERONAUTICS

-“ .

!

I I An investigatfon ie therefore being oonduoted In the Langley two-dimensional low-turbulence tUnnel8 in order t,o develop the optimum configuration of a 0.35-ChOrd s l o t t e d flap on a modified 65(,,) -111, atxfoll section and t o determine whether or n o t the dtweloped optimum f l a p configuration l e dependent upon the Reyno3.de number. Meaeurements to determine khe section pitching- tnMnent chsrscterfstioe, the effects of leading-edge roughness on the lift aharacteriatics, and, the lift characteristics f o r the flap deflected through a developed f l a p path 5 ~ y l e also bcludgd in this inveetigation a mMBoLs . .

a , aection angle of attack, degrees . * C airfoil chord section drag coefficient cd t . .

!

R Reynulds nlopber x,y horizontal and vertical positions, respectively, of t h e flap leading-edge radiue center with respect t o Upper lip of elot In percent c , positive forward of md.below s l o t l i p , respective- (fig. I) Teets were made In .the Langley two-dlnermional low-turbulence pmeeure t u x l n s l to bterrpine the scale effecta an the l i f t and drag chamrcterietfcs of t h e airfoil section with the f l a p retracted and slot sealed for Reynolds numbers ranging Frosa 3 .O x Lo 6 t 0 . 2 5 .O x 10 6 L i f t msasurements were ,=de at e Reynolds number of "9 .O x 106 t o determine t h e flap position evld deflection for highest m a x i m u m lift .d b (optinmrm configuration) The scale effects on t h e i i f t characteristics of the O p t i n n l m flap ccmfigumticn were then investigated,f!or.the same range of Reynolds numbers covered in the teats of the airfoil with

t h e flag retracted end slot aealed. The t e s t methods and the m e w

uaed in correcting the t e a t data to free-air condftione are discwered in reference 3. !Be magnitude of the correctionsused in correcting I t h e t e s t data to f'ree-air canditfona was of the order of a f e w gercont The metximum free -stream W h number attained d-ng any I of the t e s t s did not exceed 0.i8.

A i r f o i l with Flap Deflected I The 3mrernent of magimum section lift coefficient increased from. 1.84 to 1 36 as the Reynolds number was U c r sed f r o u

approxi~etsly 3.0 x 10 6 to approximately 11.0 x 10 2 as. shorn in

figure 7. The variation of incremnt of maxim section liFt .

coefficient w i t h Reynolde number, however, was l e e s than the variation of wximum eection lift coefficient w i t h Reynolds number. ! € ! h e increment of maximum soctkon l i f t coefficient for Reynol.ds.numbers r-ng From 3 .O x lo6 to 25 -0 x 106 was approximately 1.3.

I I : ?

cmcLmPom

I I I eectlon with a 0 -3i-cbrd slot+ied f l a p indicab t h e - following canclusians.

1 . The optinnun flag conffguration at high Reynolds nuaibere w a s found to be a f l a p deflection of 3 5 ' with the flap leading- edge radlua center located 1.98-percent chord behind and 3.2l-percent chord below the slot U p . The f l e p deflection wa8 lower and the f l a p was located rearward and upwd from the position found to be the optimum at a Regnoldrs number of 2.4 x LO6.

2. Shifts in the linear portion of the lift curve caused by variation in RegnoMs number,whi& oocurred only f o r the condition with the flap deflected, were either eliminated or reduced considerably .

I by altering the flap poeition.

I 3- The maximum section lift coefficient of the airfoil with the f l a p deflected in e position found to be the optimum at a, Reynolds

rnrmber of 9.0 x 10 P increased from 2 . 1 5 to 2.11 a8 the Reynolds nuniber

rJAcA RM rio. L7A24 !

Langley Memorial Aeronautical Laboratory Xational Advisory Coanaittee for Aeromutios Langley Field, Va.

" Clinton H. Dearborn Chief of E'ull-Scale Research Divisiori mPc . .

I

1. Cahfll, Jones I ? . : Two -Dimensional I~lndJPunnel Lnvestigatfon

of Four m e 8 of Hfgh-LFft Flaps on an XACA 6-210 A i r f o i l Section. NACA TBT no. 1947.

2. R ~ c ~ s z , Stanley I ? . : Two-Dimensional Wind-Tunnel hVestig8tfOn

Of Modified NACA 65 -U Airfoil W l t h 35 -Percent Chord (1121 Slotted Flap To DetermLne Optimum Flap Configuration st a

Reynolds Number Of 2 -4 Million. XACA RM Mo . L7AO2, 1946

3 . Abbott, Ira E., von Doenhoff, A l b e r t E . , and Stivers, Louis S . Jr - : Stxrmazy Of Airfoil Data. NACA ACR No. L m g , I c . . .

i t .

10 .

MACA RM No. L7A24 LE. r a d i u a r 0.842 N A T l O H u ADVDol 'ICs I of f l a p iomed by louer & m e r aurfaae surfaaa of plain airfoil.

Stationa and ordinates peraent a b f o i l a h w in Upper surfaoa fairs into plain airfoil seatloll at station 88.00 I ( a ) A i r f o i l d t h 0.350 slottedflap.

Center of flap leading-edge radius -

. ... . .. . .

. ..

. ..

I " I' . . . . . .

P NACA RM No. L7A24 Fig. 7,8 " 0 4 8 16 20 Figure 7 .- V a r i a t i o n of maximum s e o t i o n lift c o e f f i c i e n t and inareatent of maximum s e c t i o n lfit o o e f f i c i e n t w i t h Reynolds nlmber f o r a rnodFfied XACA 65(112)-111 a i r f o i l s e c t i o n with a 0.350 s l o t t e d f l a p .

I i " 0 4 8 12 16 20 24 28 x 106 Remolds nunber, R NATIONAL ADVISORY COMHITTEE Fo9 AERON*UTKS .~igure 8 .- V a r i a t i o n of s e c t i o n lift o o e f f i o l e n t at a o o n s t a n t angle of attack w i t h Repol& number for a modFfied NACA 65(1121-~1 a i r i o l l s e c t i o n with a 0 . 3 5 ~ s l o t t e d f l a p .

5 .

Source & rights

Source: ntrs.nasa.gov. Public-domain U.S. Government work (17 USC §105) — freely reproducible.

Permanent URL — we don’t break links.

Report a problem or request removal

Document details

Doc number
·
NACA-RM-L7A24
Publisher
·
NASA (NTRS)
Year
·
1947
Pages
·
19
File size
·
959 KB