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  • 8/8/2019 Hydrodynamics Effect Pipe

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    Hydrotechnical Construction, Vo l. 29, No. 7, 1995

    E X P E R IM E N T A L IN V E S T I G A T I O N S O F H Y D R O D Y N A M I C E F FE C TSIN A P IP E D U R I N G C O N N E C T I O N O F FR EE A N D P R E S S U R EF L O W S B Y A H Y D R A U L I C J U M P

    G . A . S u d o l 's k i i a n d A . M . S h v a i n s h t e in

    T h e h y d r a u l i c j u m p o c c u r r i n g d u r i n g c o n n e c t i o n o f f r ee a n d p r e s s u r e f lo w s i n a c l o s e d c o n d u i t i s a s p e c ia l t y p e o fh y d r a u l i c j u m p . A c h a r a c te r i st i c f e a t u r e o f t h is j u m p i s t h a t i t c a n o c c u r w i t h o u t p a s si n g t h r o u g h t h e c r i t ic a l d e p t h . I n t h epr es sur e sec t ion of the f low i t s r o l le r en t r a ins a cons ider ab le amou nt of a i r , w hich on a r e la t ive ly smal l d i s tance co l lec t s neart h e c e i l in g o f t h e c o n d u i t a n d m o v e s a l o n g i t t o w a r d t h e l o w e r p o o l . T h e i n d i c at e d fe a t u re s o f s u c h a j u m p c o m p a r e d w i t ha j u m p c o n n e c t i n g a r a p i d f l o w w i t h a t r a n q u il f l o w s u g g e s t t h e p o s s i b il i ty o f a d i f f e r e n c e o f t h e i r h y d r o d y n a m i ccharacter is t ics .

    T h e t y p e o f ju m p u n d e r c o n s i d e r a t io n o c c u r s m o s t o f t e n i n d i s c h a rg e p i p e s a n d t u n n e l s w h o s e m a i n g a t e s a r e l o c a t eda t the en t r ance and a r e in tended f or oper a t ing f u l l s ec t ion a t des ign d i schar ges . O n the pa th of such s t r uc tur es a hydr au l icj u m p w i t h a p r es s u r e r e g i m e d o w n s t r e a m ( H J P R ) c a n f o r m w i t h p a rt i a l o p e n i n g o f t h e g a t e s. I n t h e j u m p z o n e s u b s t a n ti a lp r e s s u r e f l u c t u a ti o n s c a n b e o b s e r v e d o n t h e p a t h o f th e c o n d u i t , d i s r eg a r d o f w h i c h c a n b e h a z a r d o u s f o r d i s c h a r g e t u n n e l s[ 1] and the mor e so f o r d i schar ge p ipes , e spec ia l ly those cons t r uc ted in the body o f ea r th dams . Th e f luc tu a t ion e ff ec t s ont h e p i p e s u r f ac e s a n d t h e v i b r a t i o n o f t h e c o n c r e t e s tr u c t u r al m e m b e r c a u s e d b y t h e m a r e t r a n s m i t t e d t o t h e e a r t h m a s s o fthe dam, w hich makes i t necessa r y to eva lua te i t s s tab i l i ty . The f i r s t s tep of such an eva lua t ion i s a de te r mina t ion of thef luc tua t ion e f f ec t s on the f low sur f aces of such a condui t . T he l i t e r a tur e conta ins few such d a ta [ 2 , 3 ] .

    E x p e r i m e n t a l i n v e s t i g a ti o n s to d e t e r m i n e p r e s s u r e f l u c tu a t i o n s o n t h e p a t h o f t h e d i s c h a r g e p i p e w i t h p a r t i a l o p e n i n g, ;i ' " e ga t~ and con nec t ion of the f r ee and pr es sur e f low by a hyd r au l ic jum p w er e ca r r ied ou t on a mo de l a t a s ca le of 1 :40

    : ~a_,,inationo f o n e o f t h e i n t e r m e d i a t e v a r i an t s o f t h e c o m b i n e d d i v e r s i o n a n d s e r v ic e p i p e o u t l e t s o f t h e U s t ' - S r e d n e k a n',~SJJ~ociectlic station.

    T h e w i d t h a n d h e i g h t o f t h e c r o s s s e c t i o n o f th e m o d e l o f t h e d i s c h a r g e s e c t io n o f t h e p a t h o f t h e p i p e o u t l et o nw h i c h t h e m e a s u r e m e n t s w e r e t a k e n w e r e 1 7 .5 a n d 3 2 . 5 c m . T h e p r e s s u r e f l u c tu a t i o n s w e r e r e c o r d e d b y m e a n s o f D D T - 1t r a n s d u c e rs a n d t h r o u g h a s t ra i n - g a u g e a m p l i fi e r w e r e r e c o r d e d o n a B r u e l l a n d K j a e r m e a s u r i n g m a g n e t i c t a p e r e c o r d e r.T h e e x p e r i m e n t a l d a t a w e r e p r o c e s se d o n a t y p e D V K c o m p u t e r . I n t h e m e a s u r i n g a n d p r o c e s s i n g s y s t e m h i g h - f r e q u e n c ynoise gr ea te r than 50 H z w as suppr es sed by means of spec ia l f i l t e r s . This c i r cums tance w as impor tan t , s ince the na tur a lf r e q u e n c y o f t h e f i rs t m o d e o f v i b r a ti o n s o f t h e 1 . 4 - cm - t h i c k o r g a n ic g l a s s s id e w a l l o f t h e m o d e l w a s a b o u t 8 0 H z . T h es c o p e o f r e a li z a t io n s o f t h e f l u c t u a t i o n p r o c e s s d u r i n g p r o c e s s i n g w a s a b o u t 3 3 0 s e c , t h e d i s c r e t i z a t io n i n t e r v a l w a s 0 . 0 2 s e c .

    The exper imenta l inves t iga t ions of the char ac te r i s t i c s o f p r es sur e f luc tua t ions in the inves t iga ted condui t conduc teda t v a l u es o f t h e F r o u d e n u m b e r f o r t h e c o n t r a c t ed s e c t i o n in f r o n t o f th e j u m p e q u a l t o 5 . 6 a n d 9 . 5 s h o w e d t h e f o l l o w i n g .

    1 . The in tens i ty of p r es sur e f luc tu a t ion (the r a t io of the s tand ar d devia t ion o to the ve lo c i ty head f o r the con t r ac tedsec t ion in f r on t o f the jum p in w hic h the ve loc i ty i s equa l to V c) d i f f e r s ins ign i f ican t ly ove r the length o f the cond ui t (F ig .l a ) . H e r e g i s th e a c c e l e r a ti o n o f g r a v i t y . T h e m a x i m u m v a l u e s o f t h is i n t e n s i t y r e a c h 0 . 0 7 - 0 , 0 9 ; t h e y a r e c l o s e t o t h e d a t ai n [ 3 ], b u t s l i g h t ly h i g h e r t h a n i n t h e e x p e r i m e n t s w i t h H J P R g i v e n i n [ 2 ]. T h e p o s i t i o n o f t h e m a x i m u m v a l u e s o f t h ein tens i t ie s o f p r es sur e f luc tua t ions over the length of the jum p in these inves t iga t ions d i f f e r somew hat , bu t f or x /h i > 8 theva lues of the in tens i t i e s a re c lose ( x i s the long i tud ina l coor d ina te r ead f r om the s ta r t o f the jum p; h j i s the h e igh t o f the jum pde te r mined as the d i f f e r ence of the he ight o f the p ipe and de pth in the cont r ac ted sec t ion hc) . The ind ica ted d i f f e r ence s canb e d u e t o c o n d i t i o n s o f s u b m e r g e n c e o f t h e j u m p a n d s h a p e o f t h e c r o s s s e c t io n o f t h e c o n d u i t s i n t h e s e i n v e s ti g a t io n s .Chan ges in f luc tua t ion in tens i ti e s a long the length of the H JPR and jump in an open chan ne l [ 4-6] d i f f e r subs tan t ia l ly . Int h e l a t te r c a s e t h e m a x i m u m i n t e n s it y v a l u e i s s l i g h t ly lo w e r a n d i t s d e c a y l o n g t h e l e n g t h o c c u r s m u c h m o r e r a p i d ly . T h es m a l l e r v a lu e o f t h e m a x i m u m v a l u e o f t h e i n t e n s i t y o f p r e s s u re f l u c t u a t io n s fo r a h y d r a u l i c j u m p i n a n o p e n c h a n n e lc o m p a r e d w i t h t h e H J P R c a n b e d u e t o t h e lo w e r v a l u e s o f t h e F r o u d e n u m b e r i n e x p e r i m e n t s c o n d u c t e d i n c lo s e d

    Translated f rom Gidrotekhnicheskoe Stroi te l 's tvo , No. 7, pp. 3-6, July, 199 5.

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  • 8/8/2019 Hydrodynamics Effect Pipe

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    e x / h j f r j g , z / h jF i g. 1 . V a r i a t i o n o f p r e s s u r e f l u c t u a t i o n i n t e n s i t i e s o n t h e b o t t o m a n dc e i l in g o f t h e c o n d u i t o v e r t h e l e n g t h o f t h e j u m p (a ) a n d h e i g h t o f t h e s i d ew a l l f o r x / h i = 3 . 3 ( b ) , v a r i a t i o n o f t h e c o e f f ic i e n t s o f s k e w n e s s a n dk u r t o s i s o v e r t h e l e n g t h o f t h e j u m p (c ) a n d ( d ), e x a m p l e s o f s p a t i a lc o r r e l a t i o n s o f p r e s s u r e f l u c t u a t i o n s o v e r th e l e n g t h o f t h e ju m p ( e) , h e i g h to f t h e s i d e w a l l f o r x /h j = 3 . 3 ( f ) , a n d a c r o s s t h e f l o w f o r x / h j = 3 . 9 ( g ).I a n d I I) c a l c u l a t e d c u r v e s f o r h i g h a n d l o w l e v e l s o f t u r b u l e n c e [ 4 ] ; 1 a n d2 ) e x p e r i m e n t a l d a t a fo r b o t t o m a n d ce i l i n g o f c o n d u i t f o r Fr c = 9 . 5 ; 3a n d 4 ) s a m e f o r F r c = 5 . 6 ; 5 a n d 6 ) s a m e o n s i d e w a l l f o r F r c = 9 . 5 a n d5 . 6 , r e s p e c t i v e l y ; 7 , 8 , a n d 9) e x p e r im e n t a l c u r v e s a c c o r d i n g t o d a t a [ 2 ,5 , 6 ] , r e s p e c t i v e l y .

    c o n d u i ts t h a n a c c o r d i n g t o t h e d a t a [ 4 - 6] . W i t h a d e c r e a s e o f t h e F r o u d e n u m b e r f o r t h e c o n t r a c t e d s e c t i o n o f a j u m p i n a nopen channe l , a s the inves t iga t ions exam ined in [7 , 8 ] ind ica te , an inc rea se , o f the ma x im um in tens i ty o f the p re s s u ref luc tua t ions to 0 . 08 -0 . 01 occu rs .2 . T h e v a l u e s o f t h e i n t e n si t ie s o f p r e s s u r e f l u c t u a ti o n s o n t h e b o t t o m a n d c e i l in g o f t h e p i p e a t t h e s a m e s i tep r a c t ic a l l y c o in c i d e , o n t h e s i d e w a l l t h e y i n c r e a s e i n th e z o n e o f " d i sp l a c e m e n t " b e t w e e n t h e f o r w a r d s t r e a m a n d r o l l e r o ft h e h y d r a u l i c j u m p ( F i g . l b ) .

    3 . T h e d i s t r i b u t io n o f t h e p r e s s u r e f l u c t u a t io n s i n t h e H J P R d i f f e r s f r o m t h e n o r m a l . T h e c o e f f i c i e n ts o f s k e w n e ssa s and ku r tos i s E reco rde d in the exp e r ime n t s ac tua l ly co inc ide on the pe r im e te r o f the condu i t . T he v a lue s o f a s a re pos i t ivea n d d e c r e a s e o v e r t h e l e n g t h f r o m t h e s t a r t o f th e j u m p , a s d i st a n c e g r e a te r t h a n ( 8 - 1 0 ) hi t h e y d o n o t e x c e e d 0 . 2 5 .A p p r o x i m a t e l y t h e s a m e c h a r a c t e r o f v a r i a t i o n o f a s w a s r e c o r d e d i n t h e i n v e s t ig a t i o n s g i v e n i n [ 5 ]. P o s i t i v e v a l u e s o f Ei n c r ea s e s o m e w h a t a l o n g t h e l e n g t h o f t h e j u m p , w h i c h i s r e la t e d t o a n i n c r e a s e o f t h e c o n t r i b u t i o n t o t h e p r e s s u r e f l u c t u at i o nb y t h e e n d o f t h e j u m p o f t h e c o m p o n e n t s f r o m d i s t u r b a n ce c a u s e d b y t h e m o v e m e n t a n d o u t f l o w o f a i r c a v i t i e s in t o t h el o w e r p o o l .

    4 . S t a b l e c o r r e l a t i o n s o f p r e s s u r e f l u c t u a t i o n s a r e t r a c e d i n t h e H J P R z o n e . T h e c o e f f i c i e n t s o f l o n g i t u d i n a lco r re l a t ions o f p re s s u re f luc tua t ions r l app roa ch ze ro on ly a t a d i s t ance g rea te r than 8h i (F ig . l e ) . T h e va lue s o f thec o r r e l a t i o n c o e f f i c i e n t r h o v e r t h e h e i g h t o f t h e c o n d u i t ( F i g . l f ) d e c r e a s e s o m e w h a t w i t h i n t h e f o r w a r d f l o w ( y i s t h ec o o r d i n a t e o r t h o g o n a l t o t h e b o t t o m o f t h e c o n d u i t ) a n d t h e n r e m a i n p r a c t i c a l ly c o n s t a n t i n t h e r o l l e r o f t h e h y d r a u l i c j u m p .T h e v a l u e s o f t h e c o r r e l a t i o n c o e f f i c i e n t o n t h e b o t t o m a n d c e i li n g o f th e c o n d u i t a t t h e s a m e s i te a r e u p t o 0 . 6 - 0 . 7 . T h ep r e s s u r e f l u c t u at i o n s o v e r t h e w i d t h o f t h e c o n d u i t a r e p r a c t i c a ll y i n p h a s e , a n d t h e v a l u e s o f t h e c o r r e l a t i o n c o e f f ic i e n tsac ros s the f low r b in F ig . t g (z i s a coo rd ina te t r ans ve rs e to the d i rec t ion o f the f low) a re c los e to u n i ty . In a l l d i rec t ionst h e v a l ue s o f t h e c o r r e l a t i o n c o e f f ic i e n t s in t h e z o n e o f t h e H J P R i n th e c o n d u i t i n v e s t i g a te d b y u s w e r e h i g h e r t h a n i n t h eU-s haped condu i t [2 ] .

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    F i g . 2 . G e n e r a l i z e d g r a p h o f t h e s p e c t r a l d e n s i t y o f p r e s s u r e f l u c t u a t i o n so n t h e b o t t o m o f t h e c o n d u i t : 1 ) z o n e o f e x p e r i m e n t a l p o i n t s f o r s i te s int h e i n i ti a l s e g m e n t o f th e j u m p b e f o r e c o n t a c t o f t h e ju m p r o ll e r w i t h t h ec o n d u i t c e i l in g ; 2 ) e x p e r i m e n t a l p o i n t s i n s e g m e n t o f c o n d u i t o p e r a t in g f u l ls e c t i o n ; 3 , 4 , a n d 5 ) c u r v e s p l o t t e d f r o m d a t a [ 7 , 9 , a n d 1 0 ] ; 6 ) c a l c u l a t e dc u r v e in a c c o r d a n c e w i t h A . M . O b u k h o v ' s d e p e n d e n c e .

    5. Th e gene r a l char ac te r o f the spec t r a l dens i ty f unc t ion of the pr es sur e f luc tua t ions g ive n in F ig . 2 in g ener a l izedcoor d in a tes i s com par able to the da ta of o the r jum p inves t iga t ions . The f o l low ing nota t ions a r e u sed in F ig . 2 : u k is theconvec t ive ve loc i ty ( eddy t r anspor t ve loc i ty) ; s i s the nor mal ized spec t r a l dens i ty ; f i s the l inea r f r equency . The va lues ofthe gene r a l ized spec t r a l dens i ty f unc t ion of p r es sur e f luc tua t ions in the in i t i a l s egm ent of the jump in F ig . 2 a r e loca ted ins idea b a n d b o u n d e d b y i t s e x t r e m e v a l u e s . I n t h e s e g m e n t l o c a te d d o w n s t r e a m o f t h e s e c t i o n i n w h i c h t h e r o l l e r o f t h e j u m p[ ou~ :e ,_ the ce i l ing and the con dui t oper a tes f u l l s ec t ion , the spec t r a l dens i ty f unc t ion i s r epr esen ted b y f i l l ed c ir c les. A s ar csa i~ ~ f ana lyz ing these da ta and compar ing them w i th the r esu l t s o f the exper iments of o the r inves t iga tor s , i t i s poss ib le:,~ de tec t ce r ta in co mm on f ea tur es and char ac te r i s t ic s o f the spec t r a l dens i ty f unc t ions o f p r es sur e f luc tua t ions :

    i n t h e i n i ti a l s e g m e n t o f th e i n v e s ti g a t ed j u m p t h e h i g h - f r e q u e n c y m a x i m u m o f t h e s p e c t r u m i s r e c o r d e d i n t h e z o n eo f S t r o u h a l n u m b e r s S h o f a b o u t 2 , b u t i s ex p r e s se d a s v i v i d l y a s f o r t h e g i v e n r e g i m e o f c o n n e c t i o n [ 9] , t h e g e n e r a l o u t l in eof the spec t r a l dens i ty f unc t ion i s even c lose r to tha t ob ta ined in the case of a sur f ace r eg ime of connec t ing f low s [ 10] ;

    i n t h e s e g m e n t o f t h e c o n d u i t o p e r at i n g fu l l s e ct i o n t h e m a x i m u m o f t h e s p e c tr a l d e n s i t y fu n c t i o n f o r S h n u m b e ra p p r o x i m a t e l y e q u a l t o 2 d e g e n e r a t e s, w h i c h i s r e l a te d t o s u p e r p o s i t i o n o f d i s tu r b a n c e s o f v a r i o u s o r i g i n ( t u rb u l e n c e c a u s e db y m o v e m e n t o f a i r c a v i t ie s ) . A p r e s s u re f l u c t u a t i o n s p e c t r u m a n a l o g o u s i n f o r m w a s o b s e r v e d i n t h e c a s e o f t h es u p e r p o s i t i o n o f d i st u r b a n c e s c a u s e d b y w h i r l p o o l s w i t h v a r i o u s a x e s o f r o t a ti o n o c c u r r i n g u n d e r c o m p l e x t h r e e -d i m e n s i o n a lcond i t ions [ 7];

    t h e m a x i m u m o f t h e s p e c tr a l d e n s i t y f u n c t i o n is r e c o r d e d a l s o i n t h e l o w - f r e q u e n c y r e g i o n f o r S h n u m b e r o f a b o u t0 .1 , bu t the cont r ibu t ion of the low - f r equen cy f luc tua t ions ( Sh < 0 .5) to the ener gy of the spec t r um i s smal l ;

    t h e r a t e o f d e c a y o f t h e s p e c t ra l d e n s i t y f u n c t io n in t h e r e g i o n o f h i g h v a l u e s o f t h e S h n u m b e r ( S h > 2 ) o c c u r s a ta s m a l l e r ra t e t h a n a c c o r d i n g t o A . M . O b u k h o v ' s f u n c t i o n a l d e p e n d e n c e F ( S ) = S h - 7 /3 .

    W h e n a n a l y z i n g t h e d a t a o n t h e s p e c tr a l d e n s i t y f u n c t io n s o f p r e s s u r e f l u c t u a t io n s , t h e e d d y t r a n s p o r t v e l o c i t y vkf i g u r e s in t h e d i m e n s i o n l e s s c o m p l e x e s l a i d o u t o n t h e c o o r d i n a t e a x e s. I t w a s d e t e r m i n e d o n t h e b a s is o f c o m p a r i n g t h eautoco r r e la t ion f unc t io n and spa t ia l cor r e la t ions of p r es sur e f luc tua t ions [ 4] and f or the g ive n condi t ion s w as about ( 0 .4-0 .6) v c .

    T h e d a t a p r e s e n t e d h e r e p e r m i t e v a l u a t in g t h e f l u c t u a t i o n c o m p o n e n t o f t h e l o a d o n t h e f l o w s u r fa c e s o f a r e c t a n g u l a rc o n d u i t i n t h e p r e s e n c e o f a h y d r a u l i c j u m p o n i ts p a t h a n d c o m p l e t e f i l li n g o f th e c o n d u i t i n t h e s t r et c h a f t e r t h e j u m p .

    .

    2.

    368

    L I T E R A T U R E C I T E D

    A . d e l C o m p o , I . F r i c a d o , a n d I . G . R o s s e l o , " S o m e p r o b l e m s i n o p e r a t i o n o f S an E s t e r b a n d a m s p i l l w a y s , " in :N in th I CO LD , V ol . 2 - R. 33 , I s tanbul ( 1967) .N . I . K u t o b a e v a , T . V . F e d u l o v a , a n d A . M . S h v a i n s h t e i n , " L a b o r a t o r y i n v e s ti g a t io n s o f h y d r o d y n a m i c e f f e ct s o nw a l l s o f t h e c l o s e d o u t l e t o f t h e T a s h k u m y r h y d r o d e v e l o p m e n t , " i n : P r o c e e d i n g s o f H y d r a u l i c E n g i n e e r i n g

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    4/4

    .

    .

    5.6.

    7.8.9.10.

    Conferences and Meetings: Methods of Study and Hydraulic Calculations o f Hydraulic Outlet Works of the B. EoVedeneev All-Russian Hydraulic Engineering Research Institute [in Russian] (1985).T. P. Provorova, A. P. Voinovich,, A. A. Ivoilov, and L. I. Naimark, "Investigation of hydrodynamic pressurefluctuations in an outlet and stilling basin for unit discharges greater than 400 m/sec," in: Proceedings of HydraulicEngineering Conferences and Meetings: Increase of the Reliability of Power Structures Under Dynamic Effects [inRussian], VNIIG im. B. E. Vedeneeva (1982).V. M. Lyatkher, Turbulence in Hydraulic Structures [in Russian], t~nergiya, Moscow (1968).O. F. Vasilev and V. I. Bukreger, "Statistical characteristics of pressure fluctuations in region of hydraulic jump,"Proc. 12th Congress IAHR, Fort Collins, Vol. 2 (1967).A. K. Khapaeva, "Hydrodynamic effect on the bottom of a flow in a hydraulic jump and behind it," in: Transactionsof the Joint Conference on Hydraulic Engineering [in Russian], VNIIG im. B. E. Vedeneeva, No. 52 (1969).A. M. Shvainshtein and A. P. Samonenko, "Pressure fluctuations on the bottom of a stilling basin located behinda tunnel," Izv. VNIIG im. B. E. Vedeneeva, 138 (1980).T. P. Provorova, "Investigation of hydrodynamic pressure fluctuations in the case of a baffle wall with a stillingbasin," Izv, VNIIG im. B. E. Vedeneeva, 172 (1983).V. V. Kamolkin, G. V. Pesin, L. B. Sapozhnikov, et al., "Investigations of pressure fluctuations on the bottom ofthe stilling basin at the Sayan hydro development," Izv. VNIIG, im. B. E. Vedeneeva, 106 (1974).V. M. Ivanov, Pressure Fluctuations on the Bottom Revetment Behind an Overflow Dam with a Bucket, CandidateDissertation Abstract, Leningrad (1983).

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