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20090015107 · Preliminary Wind-Tunnel and Flight Tests of a Balanced Split Flap, Special Report

NASA · 1934

Open the PDFPublic domain · NASATechnical Reports

Overview

One disadvantage that has been apparent in the operation of split flaps as used to date is the time and effort required to operate them. In this communication an investigation is being made of possible means for balancing them aerodynamically to make their operation easier. Several arrangements…

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11

Key points

  • The balanced split flap was tested in a wind tunnel and in flight on an F-22 airplane.
  • Wind tunnel tests indicated that the maximum lift coefficient with the balanced split flap was approximately 12 percent higher than with an unbalanced one.
  • The force required to operate the flap was found to be satisfactory at airspeeds around 65 mph.
  • Flight tests revealed that the airplane did not balance longitudinally with the controls stick free when the flap was down.
  • The use of the flap is expected to reduce the minimum speed of the airplane by about 20 percent.
Frequently asked questions
What is the purpose of the balanced split flap?

The balanced split flap is designed to make operation easier and improve aerodynamic performance.

How much higher was the maximum lift coefficient with the balanced split flap compared to the unbalanced one?

The maximum lift coefficient with the balanced split flap was approximately 12 percent higher than that of the unbalanced flap.

What were the results of the flight tests regarding flap operation?

The flight tests showed that the flap could be operated readily at airspeeds of around 65 mph, but the airplane did not balance longitudinally with the controls stick free when the flap was down.

What effect does the flap have on the minimum speed of the airplane?

The flap is expected to reduce the minimum speed of the airplane by about 20 percent, from approximately 53 mph to about 43 mph.

What were the findings regarding the force required to operate the flap?

It was found that a force of about 25 pounds was required to deflect the flap at the desired airspeed.

Document

Source of Acquls~t~on CASI Acqu~red NATIOSAL ADVISORY COUi4ITTEB FOR AZBOXAUTICS #

S P E C 1 9 L R E P O R T 23

P R E L I M I ~ A R Y WIiqD-TUMBEL AND PLIGHT TESTS OF A BALAM CED SPLIT FLAP B y Fred E, lsick and 2 l o g d L. Thompson Lsngl ey Kexaorial Aeronautical Laborat osy A u g u s t 1934 PREL I i 4 I iTARY ABD F L I G H T TESTS BALANCED SPLIT F L A P By F r e d E, Weick and Floyd L, Thompson One d i s a d v a n t a g e t h a t h a s been a p p a r e n t i n tlie opera- t i o n of s p l i t f l a p s ass u s e d t o d a t e i s t h e t i m e and e f f o r t r e q u i r e d t o o p e r a t e them. I n t h i s c o n n e c t i o n a n i n v e s t i - g a t i o n i s b e i n g made o f p o s s i b l e means f o r b a l a n c i n g them a e r o d y n ~ t ~ n i c a , l l y t o make t h e i r o p e r a t i o n e a s i e r . S e v e r a l a.rraagerne:lts h a v e bcten t e s t e d i n t h e 7 by 1 0 f o o t wind t n i i n e l , and t h o r o s u l t s of t h e wind-tunnel t o s t s a s w e l l a s p r e l i m i n a r y f l i g h t t e s t s on one of t h o more p r o m i s i n g forms a r o g i v e n i n t h i s p a p e r .

W I X D - T U E N E L TESTS &~~ar_t.tu~_-s~d__.~:?!7_gtt.g.-- T110 7 b y 1 0 f o o t wind t ~ z n n o l i s d e s c r i b e d i n r o f e r c n c o 1 t o g c t h c r w i t h t h e b a l a n c e and s t a n d a r d t e s t p r o c e d u r e . For t h e s e t e s t s a s p e c i a l model a r r a n g e n e n t mas use$- v i t L mhich c h a n g e s i n t h e f l a p s c o u l d b e mado c o n v e n i e n t l y . Tile main a i r f o i l had a chord of 20 i n c h e s and a span of 20 i n c b e s , and was l o c a t e d between t w o l o n g i t u d i n a l v e r t i c a l p l a n e s , o r end p l a t e s , e x t e n d i n g 1 4 i n c h e s ahead of and 1 4 i n c h e s b e h i n d t h e model and en- t i r e l y t h r o u g h t h e j e t v e r t i c a l l y . Thus t h e f l o w o v e r t h e a , i r f o i l w a s a p p r o x i m a t e l y two-dirneasional i n c h a r a c t e r .

The main a i r f o i l had t h e C l a r k Y s e c t i o n , and t h e d i m e n s i o n s of t h e f l a p s a r e shown i n f i g u r e 1, The e n t i r e s e r i e s of t e s t s , which a r e s t i l l under way, i n c l u d e b o t h s p l i t f l a p s and u p p e r - s u r f a c e a , i l e r o n s w i t h many h i n g e - a x i s l o c a t i o n s . O n l ~ one of t h e more p r o m i s i n g f o r m s , which h a s a l s o b e e n t e s t e d i n f l i g h t , i s c o n s i d e r e d h e r e and t h e r e s u l t s a r e compared w i t h t h o s e f o r a p l a i n u n b a l a n c e d s p l i t f l a s of t h e same s i z e .

The t e s t s were mads a t d y n a p i c p r e s s u r e c o r r e s p o n d - i n g t o a t u n n e l speed. of 8 0 m i l e s p e r hour i n s t a n d a r d ' d i r , g i v i n g a Reynolds Eunber of a p p r o x i m a t e l y 1 , 2 1 8 , 0 0 0 . Ths r e s u l t s a r e u n c o r r e c t e d f o r wind-tunnel w a l l e f f e c t .

R e s u 1 a . - Curves of l i f t , d r a g , and c e n t e r of p r e s - .

s u r e a r e g i v e n f o r t @ e b a l a n c e d s p l i t f l a p i n f i g u r e 2 and f o r t h e u n b a l a n c e d one i n f j - g a r e 3., V i t h t h e f l a p n e u t r a l t h e maximum l i f t c o e f f i c i e n t w i t h t h e p r e s e n t t e s t a r r a n g e - ment mas a p p r o x i m a t e l y t h e sa.me as t h a t w i t h t h e u s u a l mod- e l of a s p e c t r a t i o 6 b u t w i t h t h e u n b a l a n c e d s p l i t f l a p , f o r which a d i r e c t comparison i s a v a i l a b l e , i t w a s about '-5' p e r c e n t l o w e r ( r e f e r e n c e s 2 and 3 ) . I n t h e p r e s e n t t e s t s , '"the maximum l i f t c o e f f i c i e n t was 1 2 p e r c e n t h i g h e r w i t h t h e ' b k l a n c e d s p l i t f l a p t h a n v i t h t h e u n b a l a n c e d one.

The s h i f t i n t h e c e n t e r of p r e s s u r e due t o f l a p de- f l e c t i o n w a s a b o u t t h e s a v e w i t h b o t h t y p e s of f l a p . The pitching-moment c o e f f i c i e n t s a r e g i v e n f o r b o t h t y p e s i n f i g u r e 4 , and t h e hinge-moment c o e f f i c i e n t s i n f i g u r e 5.

The h i n g e moments were a b o q t 50 p e r c e n t g r e a t e r f o r t h e u n b a l a n c e d f l a p t h a n f o r t h e b a l a n c e d one.

F L I G B T TESTS A~a_raws..- The b a l a n c e d s p l i t f l a p w a s t e s t e d i n f l i g h t on a s p e c i a l wing of a n F-22 a i r p l a n e . T h i s wing i s r e c t a n g u l a r i n form w i t h a span of 30 f e e t and a chord of 6 6 i n c h e s . F o r l a t e r a l c o n t r o l t h i s wing i s f i t t e d w i t h t h e r e t r a c t a b l o a i l e r o n s d e s c r i b e d i n r e f o r o n c e 4.

The f l a p ( f i g s . 6 t o 8 ) e x t e n d e d a c r o s s t h e f u l l span of t h e wing w i t h t h e e x c e p t i o n of a 3 - f o o t c u t - o u t a t t h e c e n t e r . The arra,ngement of t h e f l a p w a s g e o m t r i c a l l y s i m - f l a r t o t h a t of t h e model. On t h e f u l l - s i z e d a i r p l a n e ' t h e f l a p c h o r d w a s 10.7 i n c h e s and t h e h i n g e a x i s w a s l o - c a t e d 1.6 i n c h e s below t h e lower s u r f a c e of t h e f l a p and 2 . 1 i n c h e s behind t h e i e a d i n g edge of t h e f l a p . The max- . i m u m d e f l e c t i a n w a s 56 . C o n t r o l of t h e f l a p w a s o b t a i n e d by means of a 22-inch l e v e r i n t h e c o c k p i t moving t h r a u g h a n a r c of 48'. T h i s l e v e r w a s c o n n e c t e d w i t h t h e fiap"by p u s h - p u l l r o d s , equipped w i t h b a l $ m b e a ~ . i n g - ' j o i n t s i n ovdor t o e l i m i n a t e f r i c t i o n . T ~ Q f l a p was c o n s t r u c t e d of L a m i - n a t e d s p r u c e w i t h q i f a b n i c c o v e r .

. ' Tests and result_g,- Tile f i r s t f l i g h t t e s t s showed -I.-- tbat t h e f o r c e r e q u i r e d t o o p e r a t e t h e f l a p w a s s a t i s f a c - t o r y . ' I t was found t h a t t h e f l a p c o u l d be o p e r a t e d r e a d i - l y a t a i r s p e e d s of t h o o r d e r of 6 5 m.p.h., which i s t h e d e s i r a b l e a i r specd f o r o p e r a t i n g t h e f l a p on t h i s a i r p l a n e .

A t t h i s s p e e d t h e p i l o v s e s t i m a t e d t h a t a f o r c e of about 2 5 pounds was r e q u i r e d t o d e f l e c t t h o f l a p . A t t h e o u t s e t t h e f l a p w a s o p e r a t e d s e v e r a l t i m e s a s t h e a i r p l s n e ap- p r o a c h e d t h e ground f o r l a n a i n g s . F a r t h e r t e s t i n g d i s - c l o s e d , however, t h a t t h e a i r p l a n e d i d n o t b a l a n c e l o n g i - t u d i n a l l y w i t h t h e c o n t r o l s t i c k f r s e when t h e f l a p w a s down and t h a t i t would be a a v i s a b l e t o c o r r e c t t h i s condi- t i o n f o r more e x t e n s i v e t e s t s .

P r e c i s e measurements t o d.etermine t h e e f f e c t of t h e f l a p on maximum l i f t i n f l i g h t h a v e n o t beon mado up t o t h e p r a s o n t t i m e . Tho r o n d i n g s o f t h e a i r - s p c o & motor set minimum s p e e d were n o t e d , b n t t h o r e i s somo doubt as t o t h e p r o c i s i o n of t h e r e a d i n g s a t v e r y l o w s p e e d s . Thc wind-tunnel r e s u l t s i n d i c a t e t h a t t h e minimum s p c c d s h o u l d b e rcdnccd nbout 20 p e r c e n t by t h e uso of t h e flap. Tho minirnum s p e c d of t h e 3'122 as flown i n t h o s o t e s t s w i t h the f l a p up i s a p p r o x i m a t e l y 53 m.p.h. Thus, t h e f l a p s h o u l d r c d u c o t h e minimum s p e c d t o a b o u t 43 m.p,h.

Tho c h i e f i n t e r e s t i n t o s t s w i t h t h o s o f l a p s l a y i n d e t e r m i n i n g t h e e f f o c t and t h e d e s i r a b i l i t y of q u i c k oper- a t i o n . I n o r d o r t o mako f u r t h e r t e s t s t o d e t e r m i n o t h e b e h a v i o r of t h e a i r p l a n e m i t h t h o f l a p o p s r a t o d q u i c k l y u n d e r v a r i o u s f l i g h t c o n d i t i o n s , i t w a s d e s i r a b l e t o ob- t a i n l o n g i t u d i n a l b a l a n c o and s t a t i c s t a b i l i t y at lorn speods w i t h t h o s t i c k f r o c . The c o n t o r of g r a v i t y of t h e a i r p l a n e mas s h i f t o d w i t h o u t s a t i s f a c t o r y r e s u l t s and a l a r g e r s t a b i l i z e r was t r i a d (25 p e r c e n t o v e r s i z e ) , Tho l a t t e r m o d i f i c a t i o n had t o be d i s c a r d e d b e c a u s e of s e v e r e t a i l v i b r a t i o n w i t h f l a p s down. A c o n d i t i o n of s t a b i l i t y w i t h s t i c k f r e e and power o f f b o t h w i t h f l a p s up and f l a p s down was f i n a l l y a t t a i n e d by a t t a c h i n g t a b s t o t h e e l e v a - t o r s , These t a b s had a c h o r d of 2 i n c h e s , a s p a n of 2 5 i n c h e s , and were d e f l e c t e d 10' m i t h r e s p e c t t o t h e e l o v a - t o r . Ths a i r p l a n e w i t h power o f f t h e n b a l a n c e d at a speod of 62 m.p,ii. m i t h t h e f l a p s down and a t a spocd of 57 m,p,h, w i t h t h e f l a p s up. I more s a t i s f a c t o r y c o n d i t i o n would be o n e i n v h i c h t h e o r d o r of t h o s p o e d s w a s r e v e r s e d , b u t w i t h t h e b a l a n c c o b t a i n e d i t w a s p o s s i b l e t o p r o c e e d w i t h t h o a d d i t i o n a l t e s t s d e s i r e d .

S e v e r a l t e s t s mere made t o d.etormine t h e b e h a v i o r of t h e a i r p l a u e when t h e f l a p was o p e r a t e d q u i c k l y . With t h e a i r p l a n e g l i d i n g s t e a d i l y at 57 m.p,h. m i t h t h e f l a p %p and s t i c k f r e e , i t =as f o u n d t h a t q u i c k o p e r a t f o n of t h e f l a p c a u s e d a smooth t r a n s i t i o n t o a s t e a d y g l i d e at 62 mop ,he w i t h c o r r e s p o n d i n g changes i n a t t i t u d e and ' f l i g h t p a t h , With t h e a i r g l a n e g l i d i n g s t e a d i l y at 62 rn,p.h.

w i t h t h e f l a p down and s t i c k f r e e , q u i c k o p e r a t i o n of t h e f l a p caused a momentary i n c r e a s e i n speed w i t h one o r two o s c i l l a t i o n s ~ . d u r i n g t h e t , r a n s i t i o n t o a s t e a d y g l i d e a t 57 m.p.h. ' . .

Another t y p e of t e s t was made w i t h t h e s t i c k h e l d back t o o b t a i n a s t e a d y g l i d e at c l o s e t o minimum speed w i t h t h e f l a p s down. The f l a p s were t h e n c l o s e d q u i c k l y and t h e s t i c k r e l e a s e d s o t h a t i t was f r e e t o assume t h e p o s i t i o n c o r r e s p o n d i n g t o a g l i d i n g speed o f 57 m.p.h.

w i t i i t h e f l a p up. T h i s p r o c e d u r e would seem t o be a b o u t t h e worst p o s s i b l e t h a t a p i l o t c o u l d a t t e m p t w i t h f l a p s f o r ' i t l e a v s s t h e a i r p l a n e f l y i n g a t a speed c o n s i d e r a b l y l e s s t h a n . t h e s t a l l i n g speed w i t h ' t h e f l a p s c l o s e d . The ' e f f e c t as o b s e r v e d by t h e p i l o t was t h a t t h e a i r p l a n e seemed t o d r o p a p p r e c i a b l y , t h e n n o s e o v e r , p i c k up speed r a p i d l y , and o s c i l l a t e s e v e r a l t i m e s b e f o r e t h e new s t e a d y glkd'ing c o n d i t i o n w i t h f l a p s up was a t t a i n e d . T h i s t y p e o f o p e r a t i o n m a s re.peated s e v e r a l t i m e s a t a n a l t i t u d e of a b o u t 500 f e e t so t h a t t h e e n s u i n g motion c o u l d b e ob- s e r v e d f f o m t h e ground. The d e c i d e d change i n a t t i t u d e and r a p i d i n c r a a s ' c i n s p e e d were o b v i o u s f e a t u r e s that c o u l d be d e t e c t e d w i t h o u t d i f f i c u l t y . The most i n t e r e s t - i n g f e a t u r e of . t h o ground o b s e r v a t i o n s c o n c e r n s t h o change i n f l i g h t p a t h . By s i g h t i n g a l o n g a s t r a i g h t e&ge h e l d p a r a l l e l t'o t h e o r i g i n a l f l i g h t p a t h w i t h f l a p down an ob- s e r v e r c o u l d t e l l t h a t t b e r e mas v e r y l i t t l e , if a n y , i n - c r e a s e i n s t e e p n e s s of t h e g l i d e a n g l e over t h a t c o r r e - s p o n d i n g t o t h e flap-down c o n d i t i o n . Tne o r i g i n a l f l i g h t p a t h was a p p a r e n t l y m a i n t a i n e d f o r a c o n s i d e r a b l e d i s t a n c e w h i l e t h e a i r p l a n e p i c k e d up s p e e d , s o t h a t t h e r a t e of ' d e s k c n t a c t u a l l y w a s c o n s i d e r a b l y i n c r e a s e d . A s t h e i n - c r e a s e i n aPr speed w a s o b s e r v e d t o be of t h a o p l e r of 50 p o r c a n t , t h e i n c r e a s e i n r a t e o f d o s c e n t , would a p p e a r t o be of t h e samo o r d e r . F o l l o w i n g t h e p h a s e of t h e motion w h e r e i n t h e speed i n c r e a s e d , t h e r e a p p e a r e d t o be a f a i r l y smooth t r a n s i t i o n t o t h e f l a t t e r g l i d i n g p a t h c o r r e s p o n d - i n g t o t h e c o n d i t i o n of f l a p s up. F u r t h e r e x p e r i m e n t s t h e n showed that by t h e u s e of t h e e l e v a t o r s t h e change i n a t t i t u d e a n d a i r s p e e d c o u l d be g r e a t l y r ~ d u c e d and t h e o s c i l l a t i o n s e l i m i n a t e d , t h e e n t i r e t r a n s i t i o n t o t h e now g l i d i n g c o n d i t i o n b e i n g made f a i r l y smoothly.

DiscussLon.- I t s h o u l d be a p p r e c i a t e d t h a t t h e a t t a i n - ment of h i n g e momeqtq. p e r m i t t i n g t h e f l a p t o b e o ~ e r a k e d q u i c k l y by means of a s i m p l e l e v e r w a s a c h i e v e d t o some e x t o n t by t h o u s e of a narrow-chord f l a p a s w e l l a s . b y o f f - s e t t i n g t h e h i n g e a x i s f r o m t h e l e a d i n g edge o f t h e f l a p .

The wind-tunnel t e s t . s i n d i c a t e , bowever,, t h a t tbg flag i s a s e f f e c t i v e a s a p l a i n s p l i t f l a p of a p p r e c i a b l y g r e a t e r c h o r d so t h a t t h e s m a l l h i n g e moments a t t a i n e d f r o m b o t h s o u r c e s a r e a t t r i b u t a b l e t o t h e b a l a n c e d t y p e of f l a p .

From t h e t e s t s of q u i c k o p e r a t i o n of t h e f l a p i t was concluded t h a t d e f l e c t i n g t h e f l a p q u i c k l y f ram i t s c l o s e d p o s i t i o n h a s no d a n z e r o u s r e s u l t s i f t h e t a i l i s d e s i g n e d t o t a k e c a r e of t h e new c o n d i t i o n s of l o n g i t u d i n a l b a l a n c e , The a t t a i n m e n t of l o n g i t u d i n a l b a l a n c e and s t a b i l i t y w i t h f l a . p s i s , however, n o t a s p e c i f i c problem concornod w i t h t h e u s e of a q u i c k l y o p e r a t e d f l a p . A sudden c l o s i n g of t h e f l a p a t mininum speed w i t h f l a p s down i s , of c o u r s e , p o t c n f i a l l y dangerous mhen performed a t vory low a l t i t u d e s .

With t h o a x o r c i s o of r e a s o n a b l e judgment, however, i t seems u n l i k e l y t h a t q u i c k o p e r a t i o n of t h o f l a p ca.n b e r e g s r d c d a,s a n y t h i n g b u t an u n q u a l i f i e d a d v a n t a g e o v e r t h o t y p e of o p e r a t i o n t h a t r c q u i r e s c o n s i d n r a b l o t i m e and e f f o r t . A t t h e F r a s c n t timo i t i s p l a n n e d t o p r o c a o d w i t h f u r t b o r t e s t s i n which a c t u x l measurements of t h e motion f o l l o w i n g q u i c k o p e r a t i o n of t h o f l a p w i l l be m a d e .

Langloy M e n o r i a l A e r o n a u t i c a l L a b o r n t o r r , N a t i o n a l Advisory C o n a i t t o o f o r A e r o n a u t i c s , L a n g l e y F i e l d , V a . , Angust 2 0 , 1934, REFEREFCXS 1. X a r r i s , Thomas A , : The 7 by 1 0 Foot Wind Tunnel of t h e B a t i o n a l Advisory Committee f o r A e r o n a u t i c s . T . R .

N o . 412, X,A,C.R., 1931, 2 . Wenzinger, C a r l J . : !find-Tunnel ideasurement s of A i r ~ o a d $ on S p l i t F l a p s . T . N . No. 498, N . A . C . A . , 1934.

3 . Weick, F r e d E . , and Wenzinger, C a r l 3 , : Wind-Tunnel R e s e a r c h Comparing L a t e r a l , C o n t r o l D e v i c e s , P a r t i c u -

l a r l y a t High Angles of A t t a c k . X I 1 - Upper-Surface

A i l e r o n s on Wings w i t h S p l i t F l a p s . T . R . No. 499, X . A . C . A . , 1934.

4 . Thonpson, Floyd 5.: R e t r a c t a b l e A i l e r o n s f o r Use w i t h Y l a p s . W ..Q,C.h. ( C o n f i d e n t i a l ) Memo. R e p o r t , Docom- b s r 1333.

N . A . C . A .

a , degrees a , degrees Figure 2.- Lift, drag, and o.p. for wing with Figure 3.- Lift, drag, and o.p. for wing with unbalanoed eplit flap.

balanced s p l i t flap.

Figure 6.- Hinge-moment ooeffioient varletion with flap defleoiiion for balanced and unbalanoed flape.

Figs. 7,8 Figure 7,- Flap retraoted.

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Document details

Doc number
·
20090015107
Publisher
·
NASA
Year
·
1934
Pages
·
11
File size
·
1.0 MB