1. Trang chủ
  2. » Thể loại khác

DSpace at VNU: Diffusion sorption experiment for studying transport properties of...

7 136 0

Đang tải... (xem toàn văn)

THÔNG TIN TÀI LIỆU

Thông tin cơ bản

Định dạng
Số trang 7
Dung lượng 2,6 MB

Nội dung

V NU JOURNAL OF SCIENCE, M athematics - Physics T.XVIII, N04 - 2002 D IF F U S IO N -S O R P T IO N E X P E R IM E N T F O R S T U D Y IN G T R A N S P O R T P I I O P E R T I E S O F 137C s A N D S5S r I N S O I L D a iig T h i P h u o n g N a m D epartm ent o f Physics, College o f Science , VN U G e r a ld K ir c h n e r Faculty o f Physics, University o f Bremen, G erm any A b s t r a c t T h e radionuclides released from nuclear weapon tests during the 1960’s and from nuclear industries may still endanger the terrestrial environment Therefore, a diffusion-sorption experiment has been carried out t.0 study the behaviour of the radionu­ clides that are of interest in safety assessments in the environmental radioactivity field such as vi7C s and 90S r T he system s studied were as close as possible to those encountered in the field T he experimental data were evaluated by numerical analysis, incorporating lin­ ear and nonlinear sorption models (six sorption isotherm models) This procedure enables us to calculate the sorption parameters of different sorption isotherm models T he parameters determinated were the diffusion and sorption properties of cesium and strontium in an Orthic Podsol soil (Germany) I I n tr o d u c tio n It is w ell recognized th a t m a n y radionuclides, p articu larly th e ca tio n ic sp ecies m i­ gra te slow ly as a result o f in tera c tio n o f radionuclidevS w ith th e so il m a trix A m ong ra­ d ion u clid es, yẦ7C s and 90S r b elo n g to the m ost h azard ou s rad ion u clid es d u e to their lon g h alflives and th eir low m igration tes (o f th e order o f cm per year Ị1 ] ) T h is im p lies th a t after m any years, th ey still rem ain w ith in th e root zon e o f th e so il w here th ey can be tak en u p by p la n ts an d later co u ld reach th e ground w ater A s a co n seq u en ce, th ey tran s­ fer in to h u m an fo o d chains an d d rin k in g w ater T herefore, it is im p o rta n t to u n derstand th e tra n sp o rt p ro cess o f l37ơ s and 90S r in the so il m atrix T h ere are various la b o to ry m eth o d s for stu d y in g tra n sp o rt o f radionuclides in soil, such as th e b a tch m eth o d and th e colum n m eth o d T h e m a in a d v a n ta g e o f th e batch m eth o d is its sim p licity H ow ever, th ere are also several d isad van tages: n o t all hydrologie flow effects are co u n ted , th e tio o f the so lu tio n to the so lid is h igh er (d u e to exp erim en tal n ecessitie s), a n d h igh er so rp tio n ca p a cities m ay be available for tracer d u e to the sh aking p rocess Ilen ce, b eca u se o f th e ex p erim en ta l co n d itio n s (w h ich differ from th o se in the field) th is m e th o d m ay give in a ccu te resu lt [2] T h e co lu m n m e th o d can elim in a te th ese d isad van tages Its m ajor d isa d v a n ta g e is its co m p lex ity an d th a t it is very tim e- sum ing [3-4]• T h e work p resented h ere appU es a d ifferent m eth o d for stu d y in g tra n sp o rt o f cesium and stro n tiu m in soil, the m od ified diffu sion -sorption ex p erim en t In th e present study, 90S r h a s b een su b stitu te d by S5S r w h ich is ch em ica lly id en tical, h as a sid era b ly shorter halflife an d can b e d etected m o re easily T h e a im s o f th e work are to: T y p e s e t by ẦẠ/ÍiS-T^X 21 D a n g T h i P h u o n g N a m , G e r a ld K ir c h n e r 22 D eterm in e diffusion and so rp tio n p aram eters for 137C s an d 85 S r Sorp tion m o d els (linear, L angniuir, Freundlich) are te ste d by fittin g th e exp erim en ­ tal d ata II E x p e r im e n ta l p r o c e d u r e T h e d iffu sion -sorp tion exp erim en t w a s perform ed u sin g O rth ic P o d so l soil sistin g o f 96.2% sand, 3.1% silt and 0.7% clay It is a typ ical soil in N o rth G erm an y [1] 37C s (cesiu m chloride in IN HC1) and 85S r (stro n tiu m chloride in aq u eou s so lu tio n ) were u sed as tracers T h e tracer so lu tio n w a s prepared by ad d in g som e sy n th e tic so lu tio n to the acid so lu tio n ta in in g the rad ion u clid es In itia l tracers co n cen tra tio n s, C o in the reservoir cell were a b ou t 70 k Bq/1 T h e arrangem ent for th e diffu sion -sorption exp erim en t is illu str a ted in F ig l R e s e r v o i r c e ll •w o "3 c M e a s u r e m e n t c e ll '5 c/5 Fig l E x p erim en tal set-u p for th e diffu sion -sorption ex p erim en t T h e soil p e lle t w as a disk w ith a diam eter o f 1.78 cm and a th ick n ess of 0.4 cm T h e d im en sion s o f th e so il p ellet w ere 2.4 cm x 0.4 cm P orosity an d d en sity o f the soil p ellet w ere 36% and 1.70 ± 0.01 g cm""3, resp ectively T h e soil p e lle t w as fixed b etw een tw o cells, th e reservoir cell o f 490 m l tain in g the tracers an d th e m easurem ent cell o f 230 m l co n ta in in g s y n th e tic so il solu tion T h e co n cen tra tio n s C o (t) o f tracers in the reservoir cell were allow ed to d ecrease w ith tim e by th e a m o u n t diffused in to soil p ellet, also by th e decay o f th e tracers In th e m easu rem en t cell sa m p les w ere w ithdraw n at certain in tervals T h e fluid o f th e m easu rem en t cell w a s rep laced b y th e sy n th etic soil solu tion , m a in ta in in g a n ear-zero cen tration A s y n th e tic so lu tio n w as selected tain in g elem en t co n cen tra tio n s w hich are as close as p o ssib le t o th e v a lu es calcu lated from th e a n a ly ses o f the so il so lu tio n sam p le in th e field Tracers diffuse from high to low cen tration T h e exp erim en t w a s perform ed at room tem p era tu re o f ° c 137C s and 855 r con­ cen tration s in so lu tio n sa m p les w ere d etected by h ig h p u rity germ an iu m - d etector S ta­ tistica l co u n tin g errors w ere in th e range o f 14-5% I I I D a ta a n a ly sis A ssu m in g a sin g le-p o ro sity m ed iu m , in w h ich th e diffusion coefficien t D is stan t in tim e an d sp ace, tran sp ort (d iffu sion is accom p an ied by sorp tion ) in th e liquid phase can b e d escrib ed by a on e-d im en sio n a l eq u ation D iffu s io n -S o r p tio n E x p e r im e n t fo r d ( x i t) dt 23 d 2C { x ) l) _ p d S ( X ) t ) dx2 € ( tgeqO , < X < L ), ỠÍ ( 1) w h ere c : co n cen tra tio n o f trace in so lu tion ; : co n cen tra tio n o f trace sorbed; p: soil density; : soil porosity; D : effectiv e diffusion coefficient; L : len g th o f s o il pellet F o r o u r e x p e rim e n ta l a rra n g e m e h t, in itia l c o n d itio n s are given as Co, 0, X = 0, X > (2) A n d th e b o u n d a ry co n d itio n s a re [3] (3) C ( L , t ) = (4) A ccording to P ic k ’s law eq (3) m ay be w ritte n as (5) T h e s o rp tio n o f th e tra c e r to th e soil m a trix is m odelled by a n o n -lin e a r first o rd er k in etic m odel = r { F ( C ) - S }, (6) w h ere r : k in e tic tim e c o n sta n t; F ( C ) : s o rp tio n iso th erm N o a n a ly tic a l so lu tio n is k now n for th is problem ; so lu tio n s a re o b ta in e d by num erical m e th o d T h is is p e rfo rm ed by usin g C ran k -N ico lso n m e th o d o f a finite difference a n d solving th e re su ltin g sy ste m o f n o n lin e a r difference e q u a tio n s by N e w to n -R a p h so n m e th o d T h is w as d escrib ed in m ore d e ta il by G K irc h n e r, [3] T h e n u m erical a lg o rith m s were b u ilt into th e n o n lin e a r c o d e P A R o f th e B M D P s ta tis tic a l code package (B M D P s ta tistic a l softw are w J D ixon, [5]) A kaike in fo rm a tio n c rite rio n A IC c a n b e u sed to fit th e so rp tio n m o d els to e x p e r­ im ental d a ta C r ite r ia b ased o n Akaike in fo rm a tio n c rite rio n A IC if m e asu re m e n t e rro rs are a d d itiv e a n d n o rm ally d is trib u te d w ith m ean zero it is given as c C obeli, [6] A I C = N in R s s +2p, w here N : n u m b e r o f d a ta p o in ts; IỈSS • re sid u al su m o f sq u ares of th e fit; D ang Thi Phuong N a m 24 G e r a ld K ir c h n e r , p : nu m ber o f p a m eters fitted A ccord in g to th e te s t, th e so rp tio n m o d el w ith th e low est v a lu e o f A I C is considered th e b e st, ta k in g in to a cco u n t th e g o o d n e ss o f th e fit as w ell as and num ber o f th e p aram eters fitted IV R e s u lts a n d d is c u s s io n T h e so rp tio n m o d e ls liste d in ta b w ere fitte d to th e ex p erim en ta l d ata for 85S r an d l37C s w ith th e linear, F reu n d lich , and L an gm u ir iso th erm a ssu m in g in sta n tan eou s and first order k in e tic so rp tio n , resp ectiv ely T h e d ifferential eq u a tio n th u s ob tain ed can b e a p p lied as a regression m o d e l w ith D }r ) Kd) K f t ì Khai) Klq ) N as fittin g param eters T h e ta b le sh o w s so rp tio n m o d e ls fitte d to th e ex p erim en ta l d a ta o f 85ỐY,137 C\s an d th e o b ta in e d v alu es o f A I C a n d R s S ' T a b l T e stin g th e fits o f th e so r p tio n m o d els for S5S r and l37C s u sin g th e Akaike criterion 137 - 85 Sr Cs Rss AIC R-ss AIC n Sorption model 116571 678 38955 1050 = K F rC N 116572 680 37722 1049 + K La2C 116576 680 38954 1052 116575 680 34353 1040 116881 684 34388 1042 72027 813 34353 1042 II No as - r{KdC dt — , ÕỈ : -S } r{K rC N - s ÔS = rf dt Ku£ + J A s can b e seen from ta b , th e b e s t fit to th e ex p erim en ta l d a ta for 85S r an d 137Cs w ere o b ta in e d a ssu m in g a lin ea r iso th erm a n d a k in etic linear iso th erm , resp ectively P a m e ters resu ltin g from fittin g th e so rp tio n m o d els for th e linear iso th erm o f S5S r an d for th e k in e tic linear iso th e r m o f l37C s are giv en in tab T a b P a m e te rs obtained by fittin g th e experim ental d ata of 86S r an d 137Cs, where th e u n c e rta in tie s of th e v alues w ere derived from th e asym ptotic sta n d a rd deviations P a m e te r N u m e r i c a l v a lu e 85S r D ( '3 c m h '1) 10.1 ± 137C s ± 1.1 k! (c m -V ) ± 1.3 ± 13.3 r (1 "6 s ' 1) in s ta n ta n e o u s ± D iffu s io n -S o r p tio n E x p e r im e n t fo r 25 The exp erim en ta l d a ta o f stro n tiu m and cesiu m co n c e n tr a tio n s diffused in to the m easu rem en t cell and th e fitted cu rv es o b ta in ed from th e reg ressio n a n a ly sis are sh ow n in fig u r e and 3, resp ectively Fig.2 C oncentrations of 85S r diffused into th e m easu rem en t cell in d ay-intervals d u rin g th e experim ent com pared to th e fit of a lin e a r so rp tio n model Fig.3 C oncentrations of 137Cs diffused into th e m e a su re m e n t cell in day-intervals d u rin g th e experim ent com pared to th e fit of a kinetic lin e a r sorption model As can be seen in figures and 3, the calculated curves are in satisfactorily agree­ ment w ith the experim ental d a ta for b o th strontium and cesium T he strontium d a ta have been corrected for its decay, since the hatf-life of 85S r is 65 days T he uncertainties of D a n g T h i P h u o n g N a m ,J G e r a l d K i r c h n e r 26 th e valu es o f th e effectiv e d iffu sio n co efficien ts are below % T h e h ig h u n certain ties o f o b ta in ed so rp tio n p a m eter m a y resu lt in large errors on in d iv id u a l d a ta p o in ts due t o th e variation o f th e co n cen tra tio n s o f cesiu m an d stro n tiu m diffused in to th e m easu rem en t cell T h e resu lts sh o w th a t th e so rp tio n iso th erm s for b o th stro n tiu m an d cesium are linear T h e in tera c tio n k in etic s for stro n tiu m to th e soil m atrix is a fast p ro cess w hile th e k in etic so rp tio n for cesiu m is slow From the v a lu e o f r (1.36 ± )* 10 “ s ” 1, the reaction tim e o f cesiu m T = In / r ca n b e c a lcu la ted to b e days T h is result, is in g o o d agreem ent w ith corresp on d in g v a lu es in th e litera tu re [7-11] T h e w id e n g e o f K d -v a lu es rep o rted in th e literatu re, up to th ree order o f m ag­ n itu d e an d m ore [ 12 ], is d u e to th e different geoch em ical factors o f th e v ariou s m a terials u sed H ow ever, our resu lts are sim ila r to th o se o f sim ilar soil and tracer co n cen tration s fou n d b y som e a u th o rs [7,12-14] In co n clu sio n , d iffu sio n -so rp tio n ex p erim en ts have a num ber o f a d v a n ta g es such as th eir ex p erim en ta l sim p lic ity a n d th e p o ssib ility to m o d el co n d itio n s th a t are close to th ose in th e field and th erefore g iv e a ccu te resu lts A lth o u g h th e d e te r m in a tio n o f th e m ig tio n rate o f stro n tiu m a n d cesiu m in soil w ill b e th e su b je c t o f a n o th er stu d y , w e can give a rough e stim a te o f th e m igration o f rad ion u clid es in so il D iffu sion is d o m in a n t w h en th e fluid v elo city is o f th e order o f cm per year In th e ca se o f lin e a r so rp tio n , th e d istrib u tio n coefficient can b e used as rough e s tim a te to p red ict th e m ig r a tio n o f rad ion u clid es in so il w hich can b e d escrib ed as: z = y /2 e D t/R d where: R d = + - K d e U sin g th e resu lts o f ou r ex p erim en t, th e m igration o f m o f e ith e r stron tiu m or cesiu m in P o d so l so il can b e e s tim a te d to take a b o u t 100 (m ore or less) years during w h ich th e a c tiv ity w o u ld b e red u ced b y a factor o f 10 T herefore, it is o f in terest to get in fo rm a tio n o n th e m ig tio n an d so rp tio n o f stro n tiu m and cesiu m in v a rio u s m aterials (soil, ro ck ) in ord er to a llo w a sa fe ty a n a ly sis in th e en viron m en tal d io a c tiv ity Geld References G K irch n er, D B a u m g a rtn er, M ig tio n R a tes o f R a d io n u clid es D e p o site d A fter th e C h ern o b y l A ccid en t in V ariou s N o rth G erm an Soils, A nalyst 1 (1 9 ) pp 175479 K B u iizl, H B a ch h u b er a n d w Schim niack, D istrib u tio n C o efficien ts o f o f 137C s, 85S r ,141 C e ,103 /ỉu ,131 J ,95rnT c in the Various of C ultivated soils in Germany, Pro­ ceedings o f the In te rn a tio n a l Sym posium on Recent Investigations in the Zone o f AeratÀon o f the Soil , M unich, O ct 1984, pp 567-568 c D S hackelford, L a b o to ry D iffu sion T estin g for W a ste D isp o sa l, A R eview , J C ontam Hydrol (1 9 ) p p 177-217 D iffu s io n - S o r p tio n E x p e r im e n t fo r 27 G K irchner, D B au m gartn er, V D elitzsch , G S ch ab l, R W elln er, L ab oratory S tu d ies on the Sorp tion B eh aviou r o f F allou t R a d io n u clid es in A gricu ltu l U sed Soils, M odel Geo-biosphere Process , (1993) pp 115-125 w J D ixon , Ỉ Ỉ MDP Statistical Sofwarc 1990, ed , U n iv e r sity o f C alifornia P ress., B erkeley 1990 C C ob elli, A R ugger, E v a lu a tio n o f A ltern a tiv e M o d el S tru ctu res M eta b o lic S y s­ tem s, Med A n d Biol Eng A nd Com put, (1 ) pp 4 -4 B T oresten felt, K A dersson , B A llard, S orp tion o f S tr o n tiu m a n d C esiu m s o n rocks and m inerals, Chemical Geology (1982) pp 123-137 G K irchner, G N ageld in ger, R W ellner, M o d ifie d D iffu sion T ech iq u e for S tu d y ­ in g N onlinear and K in etic S o rp tion an d D eso rp tio n P r o c e sse s, Radoichim A cta , (1 9 ) pp 189- 192 F B rünjes, H B ran ew itz, G K irchner, D iffusion an d D iffu sio n -C o n v ectio n E x p er­ im en ts for stu d y in g th e so rp tio n o f R a d io n u clid es in S o il, Czechoslovak Journal o f P hysics , Vol (1 9 ) p p 175-180 10 P A S in ith , M od elin g a D iffu sion -S orp tion E x p erim en t b y L in ear an d N on lin ear S orp tion Isoth erm s, Nucl.TechnoL, (1 9 ) pp -3 11 J.H oryn a, z D louhy, S tu d y on S o rp tio n P ro p er ties o f S le e te d clay, Jad Energie (1 8 ) pp 300-302 12 H B achhuber, K B u n zl and w S ch im m ack, T h e m ig tio n o f 137Cj and 5r in m u ltilayered soil, Nuclear technology, Vol (N o v 1982) p p 29 -3 13 J A D eld eb b io, S orp tion o f S tro n tiu m , S elen iu m , C a d m iu m , a n d M ercury in Soil, Radoichirn A d a , /5 ( 9 ) pp 181-186 14 K A kiba, H H a sh im o to , T K an n o, D istrib u tio n C o efficien t o f C esiu m and C ation E x ch an g e C ap a c ity of M in erals a n d R ocks, J N u c le a r S c ie n c e a n d T echnology, ( ) ( 9 ) p p 1130-1135 ... v a lu es calcu lated from th e a n a ly ses o f the so il so lu tio n sam p le in th e field Tracers diffuse from high to low cen tration T h e exp erim en t w a s perform ed at room tem p era... e fit of a kinetic lin e a r sorption model As can be seen in figures and 3, the calculated curves are in satisfactorily agree­ ment w ith the experim ental d a ta for b o th strontium and cesium... ultivated soils in Germany, Pro­ ceedings o f the In te rn a tio n a l Sym posium on Recent Investigations in the Zone o f AeratÀon o f the Soil , M unich, O ct 1984, pp 567-568 c D S hackelford,

Ngày đăng: 14/12/2017, 19:25

TÀI LIỆU CÙNG NGƯỜI DÙNG

TÀI LIỆU LIÊN QUAN