1. Trang chủ
  2. » Thể loại khác

DSpace at VNU: A three-dimentional simulation of the tidally modulated plume in the rever entrance region

13 153 0

Đang tải... (xem toàn văn)

Tài liệu hạn chế xem trước, để xem đầy đủ mời bạn chọn Tải xuống

THÔNG TIN TÀI LIỆU

Thông tin cơ bản

Định dạng
Số trang 13
Dung lượng 1,99 MB

Nội dung

DSpace at VNU: A three-dimentional simulation of the tidally modulated plume in the rever entrance region tài liệu, giáo...

VNU JOURNAL OF SCIENCE Nat S c i & Tech T XIX N01 2003 A T H R E E - D I M E N T I O N A L S IM Ư L A T IO N O F T H E T I D A L L Y M O D Ư L A T E D P L Ư M E IN T H E RIVKR E N T R A N C E R E G I O N N g u y ê n Minh H u a n D e p a r tm e n t o f H y d r o -M e te o r o lo g y a n d O c e a n o g r a p h y C o llcg e o f S c ie n c e , V N U A s t r a c t A three dim cntionaỉ mathcmatical model ùH presented to computc the ivatcr levcl, velocity and salinity distributions in stratified Coastal Lvaters a n d tid a lly m o d u la te d p lu m c o f th c rivcr en tra n cc region T h e m o d c ỉ sy s tc m c o n s is ts of hydrodynamìc, transport and turbulence closure modcls In the hydrodyn am ìc m o d e l co m p o n cn t, th e N a v ic r -S to k c s cq u a tio n s a re so lved iv ith th e h y d r o s ta tíc a s s u m p tio n (Itìd th e B o u ssin csq a p p ro xim a tio n T kc tr a n s p o r t m o d cl coruĩists o f th c ivatcr tc m p c tu rc a n d s a lin ity tra n sp o rt mocleLs T h e v a r ia tio n s in th e Lưatcr te m p c r a tu r e a n d s a lin ity in fĩu en ce th e Uỉater d e n sity , a n d in rc tu r n th e velo c ity fic ld T h e e q u a tio n s o f m o m e n tu m a n d c o n tin u ity arc soỉvccl n u m e r ic a lly u s in g th e m o d c -s p littin g tcch n iq u e A s th e tu rb u len ce m odel, a o n e-eq u a tio n k -e p siỉo n tu rb u le n c e m o d e l is a p p lied ỉn th e tra n sp o rt rnodel th e th r c e -d im c n tio n a l tíd v c c tiv c d iffu Ìo n e q u a tio n are solved The m o d el is a p p lie d to a rec ta n g le b a s in en clo sed by a Coastal b o u n d a ry a n d 'th ree opcn sea b o u n d a ries, tid a l fo r c ỉn g is im p o se d in th c fo rm o f CI /ric tio n less K elvin w a ve w ith o Ị fr c q u e n c y c n te r in g a t th e ivestcrn b o u n d a rỵ, frc sh w a te r lo a d in g w a s ta k c n in to a c c o u n t a t lo cu tio n o f one river m o u th , Uỉhich rcached a to ta l o f lOOOm1 s 1 I n t r o d u c t i o n A n e stu a r y is an a r ea o f in ter a c tio n betvveen s a lt a n d ír e s h vvater T ho nnơ)§t c o m m o n d e fin itio n u sed t h a t s t a t e s "an estu a ry is a s e m i-e n c lo s e d C oastal b o d y of vvater vvhich h a s a free c o n n e c tio n w ith the open sea and vvithin vvhich s e a w a t e r is m e a s u r a b ly d ilu te d w ith fresh w a te r derived from ia n d d r a in a g e ” T h e e s t u a r i m e inHuence may extend to nearshore Coastal waters vvhere seavvater is diluted by Ịaind d r a in a g e but b ey o n d th e c o n íìn e s o f e m e r g e n t land - m a s s e s T h e c la ss ic d e fin itio n of an estu a r y in c lu d e s t h e s e th r e e c h a r a c t e r is t u c s : s e m ie n c lo s e d , free c o n n e c tio n vvith th e open sea , and ír e s h w a te r d e r iv ed from laind d r a in a g e T hese th r e e c h a r a c te r is tic s govern th e c o n c e n tr a tio n of s e a w a t; e r , therefore, s a lin ity is th e key to e s tu a r in e c la ss iíìc a tio n T h e m ixing o f fresh V, a \ter and sea w ater p rodu ces d e n s ity g r a d ie n ts th a t d r iv e d is tin c t iv e e stu a r in e ( g r a v ita tio n a l) c irc u la tio n p a tte r n s T h e s e c irc u la tio n ancỉ s h o a lin g p a tte rn s differ w ith e a ch e s t u a r y sy stc e m accorcỉing to th e d ep th , tid a l a m p litu d e and p h a se at t h e m o u th , and th e a m o u n lt of fresh w a te r flo w in g in to th e basin 30 A t h r c c - d i m c n t i o n a l s ir n n la t ÌOĨI o f th c 31 T ho tid e t h a t a p p r o a c h e s t h e m ou th of th e e s tu a r y is th e r e s u lt o f all th e a str o n o m ic a l, m e te ọ r o lo g ic a l, se is m ic , and m a n -m a d e íactors a ffe c tin g am plit.ude and (Yequency o f t h e vvave A s th e tide e n te r s th e e s tu a r y , it is g r ea tly in flu e n c e d bv th e river d e p th , w id th , an d d isc h a r g e S u p e r im p o s e d on t h is tid a l action is th e fr e s h w a t e r /s a ltw a te r in ter a c tio n S a lt w ater w ill a d v a n c e up a s y s t e m u n til th e tidal flơw can no longer o v e rc o m e th e riverflow D e p e n d in g on th e r ela tio n s h ip betvveen tid al flow a n d river flow, th e estu a r y c a n be c la s s if ie d by its s a lin ity s tr u c tu r e a n d r e s u ltin g c irc u la tio n p a tte r n s T h e o r e t i c a l c o n s i d e r a t i o n s To s im u lt e w ind d r iv e n circ u la tio n and d e n s ity c u r r e n ts th a t occur in Coastal w a ters e s p e c ia lly in e s t u a r y s tr a tifie d bv s a lin itv and te m p e r a tu r e la y e r s c a u s in g s ig n iíìc a n t la te r a l d e n s ity g r a d ie n ts , th r e e -d im e n tio n a l m a th e m a tic a l m odel are n ecessa ry T he d e v e lo p e đ th r e e -d im e n tio n a l m a th e m a tic a l model is c a p a b le of co m p u tin g th e w a te r lev el a n d vvater particle v e lo city clistribution in th r e e princip al directio n s by s o lv in g ap p ro x im a tio n and th e th e N a v ie r -S to k e s a s s u m p tio n of e q u a tio n s ve rtica l u s in g h y d ro sta tic th e B o u s s in e s q e q u ilib r iu m , th e c o n tin u itv e q u a tio n an d e q u a tio n s of te m p e r a tu r e and s a lin ity 2.1 G o v e r n in g eiỊ uations o f the m odel T h e b a sic e q u a t io n s in th e th ree-cỉim en sion a l c a r te s ia n co o rd in a te s y s t e m are: du cu — + // — ct dx cu du d/ y\ ỉ ri ỵ r õp p tí dx õ + V — + Ví' — - A' = — Đz dv «h' cv —- + // — + V dí dx dy õv d2 —— -+ dp ~ (1 dz p(] õ y cu T ortz d_ du dz ( 1) ơy dx +~ rx r*y + õy (2 ) yy V 02 - - - + - ds PS d.S ( cỉ rx Õz Õz \ (7s -+ I I -■> + V’ — + H' -— A) c p d z dz dĩ ar õx ■H (~ :x ~ + — + Ạ — (2 ) /a H o r iz o n ta l diffusion te r m s are m e a n t to p a r a m e t e r iz e s u b g r id s c a le p r o c esses, in practice th e h o rizo n ta l d iffu s iv itv scale c o m p u ta tio n a l n o is e th e y sp a cin g s an d th e m a g n itu d e V ịị and are ta k e n Ả ịị a re u s u a lly r e q u ir e d to d am p sm a ll p ro p o rtio n a l to o f th e velo citv d e íb r m a tio n t h e h o r iz o n ta l te n s o r in griđ a n a lo g y w ith S m a g o rin ky*s (1963) p a r a m e te r is a tio n V'// = C m0Ax Ay D T a nd /.,/ = c o Ax Ay D T (2.26) 2.3 B o u n d a r V a n d i n i t i a l c o n d i t i o n s C o a sta l b o u n d a r ie s are c o n s id e r e d as im p r e g n a b le w a lls T h is m e a n s currrents, a d v e c tiv e and d iffu s iv e flu x es are s e t to zero h a t all Nguy en Minh Hucềìn u = 0, w = y = Q' V= , Juiị/ =0, ẢH— = (2.27?) Jvtỵ = , ẢH— = ( 2 Ỉ ) ôx õy O pen s e a (or river) b o u n d a r y co n d ition for the 2-1) m o d e n eed to be s u p p ỉie c d eastern b o u n d a r ie s a n d for V a t S o u t h e r n a n d n o r t h e r r n boundaries A selection can be made between different types of open b o u n d a r -y for a t western a n d u conditions T h e y h a v e th e form o f a d ia tio n co n d itio n d e r iv e d u s in g th e m e t h o d cof c h a r a c te r is tic s [H e d str o m [Rancỉall J L eV e q u e 1979), [Roed and Cooper, 1987], [R uddick, 19 95Ị] 1997] T h is is b a se d on the in te g r a tio n o f th e e q u a t io n s for t h ie incoming and o u tg o in g R ie m a n n v a r ia b le s le, s p e c ia liz e d at t h e vvestern bou n d a rv , th e n ta k e s th e form (3 ) R = u +cỊ = c F |Mr = 2cA e ,v/c coso)~t , w h e r e th e C oriolis fr e q u e n c y is e v a lu a te d at a l a t i t u d e o f , (0 is th e tiđal ír eq u e n c y , A = m a n d , r, c are th e d e p t h -in te g r a t e d a lo n g s h o r e cu r re n t, th e barotropic vvave s p e e d and th e s u r ía c e e le v a t io n T h e a m p ỉit u d e o f th o w a v e d e c r e a s e s e x p o n e n t ia llv vvith d is ta n c e to th e c o a s t vvith a d e c a v s c a le g iv e n hy th e barotropic R o ssb y r a d iu s c / f - 120 km T h e a m p lit u d e A e ' o f th e harm onic fu n ction Flíflr is storecỉ for e a ch o p e n boundary node A zero n o r m a l graciient co n d itio n is s e le c te d at th e e a s t e r n a n d northorn bouncỉaries, i.e ~ ự /

Ngày đăng: 15/12/2017, 00:53

TỪ KHÓA LIÊN QUAN

TÀI LIỆU CÙNG NGƯỜI DÙNG

TÀI LIỆU LIÊN QUAN