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Modelling the spatio-temporal evolution of H-3 in the waters of the River Tagus

Baeza, A.; García, E.; Miró, C.; Periáñez Rodríguez, Raúl

Abstract

Measurements of tritium specific activity levels and of temperatures in waters of the Torrejo´neTagus reservoir (Spain) showed that their radioactive characteristics were basically influenced by the radioactive liquid effluent from the Almaraz Nuclear Power Plant. This enters the Torrejo´neTagus reservoir via the Arrocampo cooling reservoir, which exchanges water with the first. We studied the temporal and spatial (in two dimensions) evolution of the mentioned parameters for years 1997 and 1998. The tritium levels were found to be significantly correlated with temperature. Two numerical models were constructed for a quantitative study of the tritium levels along Torrejo´n reservoir: a 1D model was used for the dispersion of tritium along the whole length of the reservoir, and a 2D depth-averaged model was used for a detailed study of the area where tritium is released into the reservoir. Both models solve the hydrodynamic equa tions, to obtain the currents induced by the exchanges of water between the reservoirs in the River Tagus and Arrocampo, and the advection/diffusion equation to calculate the dispersion of tritium. In general, the model results were in agreement with the experimental observations

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Modelling he spa io- empo al e olu ion o 3 H in he wa e s o he Ri e Tagus A. Baeza a, *, E. Ga cı ´a b , C. Mi o ´ a , R. Pe ia ´n ˜ez c a Uni e sidad de Ex emadu a, Facul ad de Ve e ina ia, Dp o. de Fı´sica, A da. Uni e sidad sn, 10071 Ca´ce es, Spain b Uni e sidad de Ex emadu a, Ingenie ı´a Te´cnica Fo es al, Dp o. de Fı´sica, 10600 Plasencia (Ca´ce es), Spain c Uni e sidad de Se illa, E.U. de Ingenie ı´a Te´cnica Ag ı´cola, Dp o. de Fı´sica Aplicada, 1, 41013 Se illa, Spain Recei ed 7 Ap il 2005; ecei ed in e ised o m 2 Oc obe 2005; accep ed 23 Oc obe 2005 A ailable online 15 Decembe 2005 Abs ac Measu emen s o i ium speci ic ac i i y le els and o empe a u es in wa e s o he To ejo ´neTagus ese oi (Spain) showed ha hei adioac i e cha ac e is ics we e basically in luenced by he adioac i e liquid e luen om he Alma az Nuclea Powe Plan . This en e s he To ejo ´neTagus ese oi ia he A ocampo cooling ese oi , which exchanges wa e wi h he i s . We s udied he empo al and spa ial (in wo dimensions) e olu ion o he men ioned pa ame e s o yea s 1997 and 1998. The i ium le els we e ound o be signi ican ly co ela ed wi h empe a u e. Two nume ical models we e cons uc ed o a quan i a i e s udy o he i ium le els along To ejo ´n ese oi : a 1D model was used o he dispe sion o i ium along he whole leng h o he ese oi , and a 2D dep h-a e aged model was used o a de ailed s udy o he a ea whe e i ium is eleased in o he ese oi . Bo h models sol e he hyd odynamic equa- ions, o ob ain he cu en s induced by he exchanges o wa e be ween he ese oi s in he Ri e Tagus and A ocampo, and he ad ec ion/di usion equa ion o calcula e he dispe sion o i ium. In gene al, he model esul s we e in ag eemen wi h he expe imen al obse a ions. Ó2005 Else ie L d. All igh s ese ed. Keywo ds: Rese oi wa e ; T i ium; Tempe a u e; Nume ical modelling; Dispe sion * Co esponding au ho . Tel./ ax: þ34 927 25 71 53. E-mail add ess: [email p o ec ed]s (A. Baeza). 0265-931X/$ - see on ma e Ó2005 Else ie L d. All igh s ese ed. doi:10.1016/j.jen ad.2005.10.004 Jou nal o En i onmen al Radioac i i y 86 (2006) 367e383 www.else ie .com/loca e/jen ad 1. In oduc ion The quali y o he plane wa e s no ably in luence hei use, wi h he p esence o adionu- clides being one o he limi ing ac o s. In his sense, he s udy o he i ium con en o di e en wa e s has a h ee old in e es . Fi s ly, i s uni e sali y, since i ium le els due o na u al o igins (Kau man and Libby, 1954) may be aised by se e al o de s o magni ude by an an h opogenic componen (UNSCEAR, 1988; IAEA, 1990; Okada and Momoshima, 1993). Secondly, i s adio- oxici y, which, while ela i ely low in compa ison wi h ha o o he adionuclides, is 25 000 imes g ea e when he 3 H is in he o m o HTO ins ead o HT (ICRP, 1978). Thi dly, he p ac- ically indis inguishabili y o hyd aulic sys ems o i ia ed wa e om un i ia ed wa e (Thi- bodeaux, 1979), so ha his adionuclide may be a good pa ame e o s udying he dynamics o wa e masses (Fon es, 1983a,b; Baeza e al., 2002), and in pa icula o s udying he spa ial and empo al dis ibu ion o o he subs ances con ained in hem, whe he conse a i e o no . One o he Ibe ian Peninsula hyd ological sys ems ha is mos a ec ed by he p esence o i ium is he Ri e Tagus. The p incipal eason is ha h ee nuclea powe plan s use i s wa e o cooling (CSN, 1998). I s cou se is highly egula ed by an almos comple ely coupled se ies o ese oi s, which a e especially impo an in he i e passage h ough he egions o Ex em- adu a (Spain) and he Alen ejo (Po ugal), wi h i e ese oi s in 200 km. The au ho s s udied p e iously, o he yea s 1994e1996, he basic aspec s o he i ium’s spa ial and empo al e o- lu ion (Baeza e al., 1997), including a ious simple models ha allowed us o unde s and ce - ain ace s o i s dynamics, such as i s mean ansi speed (Baeza e al., 2001, 2004). One ac deduced was he impo ance o To ejo ´n ese oi in unde s anding he spa ial and empo al e olu ion o i ium in his pa o he Ri e Tagus, since he wa e is used no only o hyd oelec ic powe p oduc ion and i iga ion, bu also o cool he Alma az Nuclea Powe Plan (hence o h, ANPP) h ough wa e exchanges wi h A ocampo ese oi . In he p esen wo k, we s udy in de ail he in luence o his wa e exchange on he dis ibu ion o i ium in To ejo ´n ese oi , using da a o yea s 1997 and 1998. To his end, we collec ed mon hly wa e samples, in which we de e mined hei empe a u es simul aneously wi h he collec ion. In his way we we e able o analyze bo h he spa ial dis ibu ion o i ium le els in wo dimen- sions in To ejo ´n ese oi , ans e sally and longi udinally, and hei empo al e olu ion. The cu en s caused by he exchange o wa e be ween he di e en ese oi s in his pa o he Ri e Tagus make i di icul o gi e a de ailed quan i a i e in e p e a ion o he measu ed i ium le els, in a o m allowing p edic ions o hei u u e e olu ion. A p e equisi e is o con- s uc app op ia e models o To ejo ´n ese oi . We made a i s app oxima ion by using simple box models o simula e he empo al e olu ion o i ium le els in he A ocampo (Baeza e al., 1997) and To ejo ´n(Baeza e al., 2001) ese oi s, in pa icula s udying he a ea whe e he exchange o wa e wi h he A ocampo ese oi akes place. The p esen wo k desc ibes he de elopmen o wo new nume ical models o he To ejo ´n ese oi . The i s is a one-dimen- sional model cons uc ed o ep oduce he la ge scale dispe sion o i ium, co e ing he o al leng h o he ci ed ese oi . This model canno , howe e , desc ibe he dispe sion o i ium a a small scale, in pa icula in he a ea o he discha ges om A ocampo ese oi . A highe esolu ion wo-dimensional dep h-a e aged model was he e o e cons uc ed o his a ea. The ad ance ep esen ed by hese models is ha hey a e physical models in which he ins an- aneous cu en s a e ob ained o each poin o he To ejo ´n ese oi and o each ins an o ime. These cu en s a e hen used o calcula e he i ium dispe sion. Hence, he i ium con- cen a ions may be calcula ed o any posi ion and ime in his ese oi . 368 A. Baeza e al. / J. En i on. Radioac i i y 86 (2006) 367e383 2. Expe imen al 2.1. S udy a ea The Ri e Tagus has i s sou ce in he Sie a de Alba acı ´n (Spain), and i s mou h in Lisbon (Po ugal). I s o al leng h is 1107 km (Fig. 1). The a ea o he Tagus basin is abou 8.1 10 4 km 2 , o which 69% is in Spain. The ANPP, wi h wo 930 MWe PWR- ype uni s is loca ed on he i e igh bank, in he egion o Ex emadu a and 180 km wes esou hwes o Mad id. The Ri e Tagus ecei es discha ges om he ANPP (Baeza e al., 1991) and om o he wo nuclea powe plan s loca ed below 300 km ups eam eJose ´Cab e a and T illo eas well as se e al smalle con ibu ions om a signi ican numbe o labo a o ies and hospi als (CSN, 1998). The low egime o he Ri e Tagus is con olled h ough a chain o ese oi s. One o hem, in he egion o Ex emadu a (Fig. 1), is, in cubic hec ome es (1 hm 3 ¼10 6 m 3 ), he 166 hm 3 capaci y To ejo ´n ese oi , which is he objec o he de ailed s udy o he p esen wo k. I is 42 km long, wi h a mean wid h o 130 m and a mean dep h o 20 m. Immedia ely ups eam, he 500 hm 3 capaci y Valdecan ˜as ese oi is loca ed. The Alca ´n a a ese oi , wi h a no mal ol- ume o 1600 hm 3 , is si ua ed downs eam om To ejo ´n. The wa e o To ejo ´n ese oi is pe- iodically pa ially exchanged wi h ha o A ocampo, since he la e is used as he ANPP’s Fig. 1. Map o he Ri e Tagus wi h he loca ions o he sampling poin s. The loca ion o he dam o each ese oi is indica ed by <. 369A. Baeza e al. / J. En i on. Radioac i i y 86 (2006) 367e383 seconda y cooling ci cui . The pu pose o he exchange is o main ain A ocampo’s olume p ac ically cons an a 35 hm 3 (ANPP, 1998) and i s wa e empe a u e su icien ly low o ul il i s cooling unc ion. The lowe pa o Fig. 2 shows he empo al e olu ion o he lows be ween he A ocampo and To ejo ´n ese oi s. The s ong 12-mon h pe iod seasonali y o hese exchanges, as has been desc ibed in p e ious s udies (Baeza e al., 2001), is obse ed. The uppe pa o he Fig. 2 shows he mon hly discha ges o wa e be ween he Tagus ese oi s p esen in Fig. 1, i.e., om Valdecan ˜as o To ejo ´n, and om he la e o Alca ´n a a. I can be seen ha he man- agemen o he discha ges be ween hese h ee ese oi s is pe ec ly coupled, which, as was indica ed abo e, is a common cha ac e is ic o all he Ri e Tagus ese oi s. On he o he hand, his managemen is adically di e en om ha be ween To ejo ´n and A ocampo, since he obse ed seasonali y in his case is condi ioned by he a ailabili y o wa e in he Tagus Ri e , which in u n is ela ed o he in ensi y and equency o ain alls in he a ea. 2.2. Sampling Two sampling p og ams eone mon hly and he o he in ensi e ewe e ca ied ou in 1997 and 1998 in he abo e desc ibed s udy a ea. The in ensi e p og am o sampling was designed o de e mine he spa ial dis ibu ion o i ium le els in wo dimensions in To ejo ´n ese oi : lon- gi udinally, o 17 sampling poin s dis ibu ed along he leng h o he ese oi , and ans e - sally, in he cen e and on he wo banks o he ese oi o each o hose 17 poin s. The mon hly p og am was o allow us o analyze he empo al e olu ion on he basis o mon hly DISCHARGES 0 500 1000 1500 1 3 5 7 9 11 13 15 17 19 21 23 1997-1998 1357 9 11 13 15 17 19 21 23 1997-1998 (hm 3 ) (hm 3 ) Valdecañas To ejón 0 25 50 75 100 A ocampo o To ejón To ejón o A ocampo Fig. 2. Uppe pa : mon hly discha ges o wa e om Valdecan ˜as o To ejo ´n, con inuous line, and om To ejo ´n o Alca ´n a a, do ed line. Lowe pa : mon hly exchange o wa e om A ocampo ese oi o To ejo ´n ese oi , con in- uous line, and om To ejo ´n o A ocampo ese oi , do ed line. 370 A. Baeza e al. / J. En i on. Radioac i i y 86 (2006) 367e383 eco ds a h ee o he a o emen ioned sampling poin s in To ejo ´n ese oi and a ano he poin in A ocampo ese oi . Wa e empe a u e was simul aneously eco ded wi h each sam- ple collec ion. 2.2.1. Mon hly sampling E e y mon h, su ace wa e samples we e collec ed a he h ee sampling poin s o he To - ejo ´n ese oi iden i ied as 1, 7, and 8 in Fig. 1, and a one sampling poin o he A ocampo ese oi iden i ied as A in he igu e. As was no ed abo e, A ocampo is he cooling ese oi o he ANPP. The e is a cons an o ced ci cula ion o wa e a a a e o 88 m 3 /s a ound he sepa a ion dyke cons uc ed in he cen e o he ese oi . As a esul , i s wa e has pe ec ly homogeneous physicochemical p ope ies (Baeza e al., 1991), so ha poin A is en i ely ep- esen a i e o he cha ac e is ics o wa e in he ese oi . The loca ions o poin s 1, 7, and 8 in To ejo ´n ese oi a e he ollowing. Poin 1 is some 10 m om he To ejo ´n dam, on he le bank o he Tagus. Poin 7 is downs eam he A ocampo dam and close o he ou le om ha ese oi in o To ejo ´n, on he igh bank o he Tagus. Finally, poin 8 is some 400 m ups eam o poin 7, on he le bank o he i e and clea ly in he opposi e di ec ion o he na u al low o he wa e . These las wo poin s a e logically hose ha will be mos in ensely a ec ed by he mixing o wa e s be ween he To ejo ´n and A ocampo ese oi s, which, as we shall see below, ha e e y di e en adiological and he mal cha ac e is ics. 2.2.2. In ensi e sampling In ensi e sampling was ca ied ou on wo speci ic da es: 1997-08-01 and 1998-02-12. As can be seen in he lowe pa o Fig. 2, he o me da e co esponds o he ime o yea when he exchange o wa e be ween To ejo ´n and A ocampo ese oi s is maximum, while he la e is ep esen a i e o he ime o yea when he olumes o exchanged wa e a e ela- i ely low. On bo h da es, su ace wa e samples we e collec ed in a numbe o longi udinal and ans e sal ansec s o he To ejo ´n ese oi . Fig. 1 shows he loca ion o he poin s in he h ee longi udinal ansec s, co e ing he 42 km leng h o he ese oi . The sepa a ion o hese poin s was kep as homogeneous as possible, excep o a zone o he ese oi ha is especially p o ec ed because o i s wildli e. The numbe o sampling poin s on he 1998-02-12 da e was inc eased in ligh o he esul s o he analysis o he 1997-08-01 samples. 2.3. Analy ical me hods A each sampling poin , 1.5 L o wa e was collec ed in polye hylene bo les, and empe a- u e was measu ed wi h a p ecision o 0.1 C. A e anspo o he labo a o y, he samples we e il e ed h ough 0.45 mm po e il e s p io o hei p epa a ion o 3 H assay. Fo he i ium assay, a 50 mL aliquo was aken and subjec ed o a p ocess o simple dis- illa ion o elimina e colou a ion, o ganic ma e , and sal s ha migh in e e e wi h he analysis. The dis illed sample was hen mixed wi h a scin illa ion solu ion o Op iphase Hisa e 3 om LKB-Wallac a a sample/scin illa o a io o 8/12 (Scho ¨nho e and Hen ich, 1987)in20mL e lon-coa ed polye hylene ials. T i ium con en was de e mined using a Quan ulus-1220, LKB-Wallac, liquid-scin illa ion alphaebe a spec ome e . The quenching calib a ion was pe - o med wi h i ium s anda ds quenched o inc easing deg ees wi h CCl 4 . The backg ound in he egion o he i ium b-emission was o he o de o 1.5 cpm. The sys ema ically used coun - ing ime was 1000 min (200 min 5 measu emen cycles). The esul ing Lowe De ec ion 371A. Baeza e al. / J. En i on. Radioac i i y 86 (2006) 367e383 Limi a a 95% con idence o i ium was 0.5 Bq/L and he igu e o me i , (e iciency) 2 /back- g ound, was 320 (Baeza e al., 1999). 3. Resul s and discussion 3.1. Tempo al e olu ion (1997e1998) Fig. 3 shows he empo al e olu ion o 3 H le els and he empe a u e a he su ace wa e o he sampling poin s iden i ied in Fig. 1 as 1, 7, and 8, belonging o To ejo ´n ese oi , and poin A in A ocampo ese oi . Table 1 lis s he mean alues and anges eco ded a hese sampling poin s o he ci ed a iables e i ium and empe a u e. The ollowing esul s s and ou . The highes ac i i y le els we e eco ded a poin A, as was o be expec ed since his is he cooling ese oi o he ANPP. Ac i i y le els and hei empo al e olu ion a e consis en wi h he indings o p e ious s udies (Baeza e al., 2001). The obse ed empo al e olu ion is a con- sequence o he managemen o hese wa e s, whose egime o exchange wi h hose o he To - ejo ´n ese oi (see lowe pa o Fig. 2) is condi ioned by he maximum empe a u e ha he wa e can each o be used o cool he ANPP. Thus, poin A no only had he highes empe - a u es o all he s udy a ea, bu i also had he na owes ange o empe a u es as well. This is because in he cold mon hs o he yea , when i is unnecessa y o exchange wa e in o de o sa is y he he mal equi emen s, i s empe a u e alls o less han ha o he To ejo ´n ese oi wa e s. The ei e a ed use o he A ocampo wa e as coolan du ing win e is also he eason why 3 H le els a poin A we e highe in hese mon hs. In pa icula , he e was a signi ican neg- a i e co ela ion be ween i ium le els and empe a u e a poin A (see he las ow o Table 1). Fo he h ee poin s sampled mon hly in he To ejo ´n ese oi epoin s 1, 7, and 8 ebo h i ium le els and empe a u e dec eased om poin 7 o 8, and om he las o poin 1. This is eadily unde s andable gi en he spa ial loca ion o hese h ee poin s (see Fig. 1) ela i e o he 0 50 100 150 200 250 300 0 10 20 30 40 Sampling poin A Sampling poin 7 0 100 200 300 400 500 1357911131517192123 1997-1998 1357911131517192123 1997-1998 1 3 5 7 9 11 13 15 17 19 21 23 1997-1998 1 3 5 7 9 11 13 15 17 19 21 23 1997-1998 3H (Bq·L-1) 3H (Bq·L-1) 3H (Bq·L-1) 3H (Bq·L-1) 0 10 20 30 T (ºC) T (ºC) T (ºC) T (ºC) H-3 T H-3 T H-3 T H-3 T 600 40 Sampling poin 8 0 50 100 150 200 250 300 Sampling poin 1 0 20 40 60 80 0 10 20 30 40 0 10 20 30 40 Fig. 3. Speci ic ac i i y o i ium and empe a u e measu ed du ing 1997e1998 a sampling poin s A, 1, 7, and 8 o he s udy a ea. 372 A. Baeza e al. / J. En i on. Radioac i i y 86 (2006) 367e383 local sou ce o i ium and hea in o To ejo ´n ese oi , i.e., he discha ge om he A ocampo ese oi . Local empo a y inc eases in ac i i y we e di ec ly co ela ed wi h inc eases in he exchange o wa e be ween he A ocampo and To ejo ´n ese oi s (see lowe pa o Fig. 2), and he e o e had a s a is ically signi ican posi i e co ela ion wi h ises in To ejo ´n ese oi wa e empe a u e (see he las ow o Table 1). These empe a u e inc eases o cou se ha e a na u al componen du ing he ho mon hs, ein o ced by he ci ed exchanges wi h he ho e wa e in A ocampo ese oi . The coupled egula ed ansi o wa e in his zone o he Ri e Tagus (see uppe pa o Fig. 2) is ul ima ely esponsible o he anspo o i ium discha ged in o he To ejo ´n ese oi o wa e s below To ejo ´n dam. This ansi occu s p e - e en ially du ing win e , so ha i ium is sp ead ou along he men ioned ese oi du ing he summe mon hs. 3.2. Spa ial e olu ion To check he e aci y o he o egoing s a emen , we pe o med an in ensi e s udy on he spa ial dis ibu ion o i ium and empe a u e on wo da es ha we e clea ly iden i iable wi h he p e iously ypi ied cha ac e is ics o he mon hs o win e and o summe . Resul s a e p esen ed in Table 2. The able lis s, i s ly, he dis ance o he 17 poin s selec ed along he leng h o he To ejo ´n ese oi (see Fig. 1) om he ou le o he discha ges om he A - ocampo ese oi (poin 7). Secondly, o each o he wo sampling da es and each sampling poin , i lis s he 3 H le el and, in pa en heses, wa e empe a u e in he cen e and nea he banks. I can be obse ed ha he esul s we e adically di e en in he condi ions iden i ied as summe (sampling da e 1997-08-01) and win e (sampling da e 1998-02-19). The summe sam- ples showed a good ans e sal mixing in bo h i ium le els and empe a u es a each sampling poin . Indeed, he maximum ela i e ans e sal a ia ion was 13.8% o 3 H and 5.2% o em- pe a u e, bo h co esponding o poin 17. Likewise, he o e all spa ial homogenei y was also e y signi ican . In pa icula , omi ing he ac i i ies and empe a u es measu ed a poin 17 which is 12.4 km away in he opposi e di ec ion o no mal wa e low in he ese oi , we can conside ha he es o he ese oi has a well de ined i ium le el and empe a u e in he condi ions ha we e iden i ied as summe . In pa icula , o ha sampling da e, he alues we e 56.6 3.2 (SD) Bq/L and 29.2 1.5 (SD) C, espec i ely. The wo pa ame e s we e closely co ela ed, wi h a co ela ion coe icien o 0.880 a a signi icance le el quan i ied by he alue o he pa ame e p¼510 4 . Table 1 Mean alues and anges o i ium and empe a u e eco ded du ing yea s 1997 and 1998 in wa e s o A ocampo es- e oi (poin A), and To ejo ´n ese oi (poin s 1, 7, and 8) Sampling poin A 1 7 8 3 HSD (Bq/L) 270 144 22 19 101 77 57 63 Range 3 H (Bq/L) 59e496 1.4e6.0 2.4e243 1.2e199 TSD (C) 28 5185218207 Range T(C) 19e36.2 9e26.5 10e30.5 10e28.5 Co ela ion 3 HeT(signi icance le el) 0.774 (<0.0001) 0.676 (0.0003) 0.484 (0.0165) 0.711 (<0.0001) De ails o he co ela ion be ween hese wo pa ame e s, a he ou sampling poin s ha we e selec ed o he s udy o he empo al e olu ion, a e also gi en. 373A. Baeza e al. / J. En i on. Radioac i i y 86 (2006) 367e383 Table 2 De ails o he wo in ensi e sampling campaigns, iden i ying he dis ance (m) o each sampling poin om he ou le o wa e discha ged om A ocampo ese oi in o To ejo ´n ese oi No a ion Dis ance (m) Sampling 1997-08-01 Sampling 1998-02-19 Le side Cen um Righ side Le side Cen um Righ side 1þ28 600 53 3 (26.0) 54 3 (26.5) 56 3 (26.0) 1.5 1.5 (11.5) 1.5 1.5 (11.5) 1.5 1.5 (11.5) 2þ13 100 58 3 (27.0) 58 3 (27.0) 61 4 (27.0) 17.5 2.0 (10.5) 17.7 2.0 (10.5) 17.8 2.0 (10.5) 3þ2600 56 3 (28.7) 55 3 (29.0) 56 3 (29.0) 34 3 (11.0) 16.6 1.9 (10.0) 10.7 1.7 (11.0) 4þ1600 57 3 (29.0) 58 3 (29.5) 57 3 (29.0) 44 3 (11.5) 48 3 (12.0) 7.6 1.7 (11.0) 5þ600 57 3 (29.5) 58 3 (29.5) 60 4 (30.0) 32 3 (12.0) 87 5 (13.0) 58 4 (12.0) 6þ300 53 3 (30.2) 57 3 (30.5) 56 3 (30.0) 88 5 (13.5) 111 6 (14.0) 81 5 (13.0) 70 594 (31.0) 58 3 (31.5) 55 3 (32.0) 3.7 1.6 (10.0) 229 11 (18.5) 371 18 (24.0) 8400 58 3 (30.5) 54 3 (30.5) 55 3 (30.5) 1.6 1.5 (10.0) 2.5 1.5 (10.0) 1.5 1.5 (9.5) 92400 54 3 (29.5) 56 3 (29.5) 53 3 (29.5) 3.9 1.6 (10.5) 5.0 1.7 (9.5) 4.4 1.6 (10.0) 10 2900 52 3 (28.0) 51 3 (29.0) 53 3 (29.0) 3.7 1.5 (11.0) 3.8 1.5 (10.0) 1.5 1.5 (9.5) 11 3900 No da a No da a No da a 3.3 1.6 (10.0) 3.0 1.5 (10.0) 2.0 1.5 (10.0) 12 4900 60 4 (30.3) 67 4 (30.2) 61 4 (29.0) 2.2 1.5 (9.5) 2.5 1.5 (9.5) 2.4 1.5 (9.5) 13 6400 No da a No da a No da a 2.9 1.5 (9.5) 3.8 1.5 (9.5) 2.8 1.6 (9.5) 14 7900 No da a No da a No da a 2.2 1.5 (9.5) 2.2 1.5 (9.5) 2.2 1.5 (9.5) 15 8900 No da a No da a No da a 2.2 2.0 (10.5) 1.5 1.5 (9.5) 2.5 1.5 (9.5) 16 11 400 No da a No da a No da a 1.5 1.5 (9.5) 1.5 1.5 (9.5) 2.6 1.6 (9.5) 17 12 400 2.2 1.3 (19.0) 2.0 1.3 (19.0) 2.3 1.3 (20.0) 1.5 1.5 (9.5) 1.5 1.5 (9.5) 2.8 1.6 (9.5) The sign þo indica es whe he i is in he same di ec ion o he opposed one, espec i ely, as he no mal ad ance o he wa e in he To ejo ´n ese oi . The able lis s, o each o he wo sampling da es, he 3 H le els (Bq/L) and, in pa en heses, he empe a u e (C) o he su ace wa e close o he wo banks and in he cen e o he ese oi . 374 A. Baeza e al. / J. En i on. Radioac i i y 86 (2006) 367e383 Wi h espec o he spa ial dis ibu ion in he To ejo ´n ese oi de e mined on he sampling da e ypical o win e condi ions, i.e., when he e was a small low o ela i ely wa m wa e om he A ocampo ese oi con aining ela i ely high le els o i ium, as well as a la ge wa- e low in he di ec ion o he na u al cu en in his ac o he Ri e Tagus, he ollowing ac s may be obse ed. Fi s ly, he adioac i e and he mal con ibu ions om he A ocampo dis- cha ges we e only no able in a limi ed po ion o he To ejo ´n ese oi . This zone was in he di ec ion o he na u al ad ance o he wa e , also a ou ed by he di ec ion o he A o- campo discha ge canal on he igh bank o he Ri e Tagus a poin 7. One obse es in Table 2 ha i was p ecisely a ha poin whe e he highes empe a u e and 3 H ac i i y we e de ec ed. Bo h he ans e se and he longi udinal homogenei ies o hese pa ame e s in he To ejo ´n es- e oi wa e ha e disappea ed unde he ope a ing condi ions ha we e iden i ied as being yp- ical o win e . Indeed, du ing hese win e mon hs, he impac o he A ocampo discha ges was only pa ially de ec able downs eam om he ou le poin in o he To ejo ´n ese oi . I could no e en be de ec ed a he head o he ese oi , as indeed was he case on he summe da e o ou in ensi e sampling. None heless, he wo pa ame e s e 3 H ac i i y and empe a u e ewe e again pe ec ly co ela ed, e lec ing hei common o igin in he discha ges om A ocampo in o he To ejo ´n ese oi . The co ela ion coe icien was 0.974, wi h a signi icance le el quan i ied by he alue o he pa ame e p¼10 4 . 4. The modelling s udy 4.1. 1D model The use o a longi udinal model o s udy he dispe sion o i ium in he whole To ejo ´n ese oi is jus i ied by i s na owness and shallowness ela i e o i s leng h (see he Sec ion 2.1). Also, discha ges om A ocampo a e designed o achie e a apid mixing o he pollu- an s bo h in dep h and ans e sally. Thus, we a e dealing, essen ially, wi h a one-dimensional dispe sion p oblem. Indeed, 1D models ha e been ound o be adequa e ools o s udying he dispe sion o pollu an s in channeled egions and i e s (Ab il and Abdel-Aal, 2000; Ab il e al., 2000; P andle, 1974). The hyd odynamic equa ions a e sol ed o ob ain he cu en s along he ese oi o he ime pe iod o in e es . In he p esen case, he ad ec ion/di usion dispe sion equa ion o i ium is sol ed simul aneously. The 1D hyd odynamic equa ions a e (P andle, 1974) dS z þ ðAuÞ xdxQ¼0 u þu u xþg z xþCd ujuj hþz¼0 whe e Sis he ho izon al su ace a ea, z he heigh o he wa e su ace abo e he mean le el, u he wa e eloci y along he xdi ec ion, A he c oss-sec ion a ea o he ese oi , g he accel- e a ion due o g a i y, Q he ex e nal low o wa e en e ing/lea ing he ese oi a each poin , and ha dep h pa ame e de ined as h¼A/bwhe e bis he wid h o he ese oi . The bed ic- ion coe icien is de ined as Cd¼g C2 h 375A. Baeza e al. / J. En i on. Radioac i i y 86 (2006) 367e383 e olu ion o he le els o i ium in he ese oi s o A ocampo and To ejo ´n hence depends s ongly on he managemen o hei wa e s. The empo al e olu ion o he wa e empe a u e is also condi ioned by he na u al e olu ion o he en i onmen al empe a u e. The wo magni- udes consequen ly p esen ed seasonal a ia ions wi h an annual pe iod, which we e six mon hs ou o phase in he A ocampo ese oi , and pe ec ly synch onized a he h ee sampling poin s ha we e sys ema ically analyzed in he To ejo ´n ese oi . Fo he s udy o he spa ial e olu ion o i ium in he To ejo ´n ese oi , we ca ied ou in- ensi e sampling a nume ous poin s o he ese oi on wo da es clea ly ypical o win e and o summe . In win e , due o he minimal exchange o wa e wi h he A ocampo ese oi and o he la ge wa e low in he na u al di ec ion o he Ri e Tagus wa e s, he To ejo ´n ese oi was ound o beha e in a o m simila o a i e wi h a quasi-na u al low egime. Consequen ly, he ela i ely insigni ican inpu s o i ium and hea om he A ocampo ese oi undamen- ally a ec ed he a ea close o and downs eam om he discha ge poin (poin 7 in ou s udy), wi h majo ans e se and longi udinal g adien s in bo h empe a u e and i ium ac i i y. On he con a y, in summe , he To ejo ´n ese oi was ound o beha e in a o m simila o a lake, since he e we e minimal lows o wa e om Valdecan ˜as ups eam, and in o Alca ´n a a downs eam. The exchange o wa e wi h he A ocampo ese oi , whe e he i ium le els and he empe a u e a e highe , was maximal a ha ime, howe e . In hese condi ions, bo h he 3 H and he hea di used p ac ically o e he whole To ejo ´n ese oi , wi h he consequen longi- udinal and ans e sal homogeniza ion o hese wo magni udes. A 1D model o he To ejo ´n ese oi was de eloped o s udy he beha iou o i ium. In gene al, he model yielded a empo al e olu ion o i ium speci ic ac i i ies along he ese oi , and i ium p o iles along he leng h o he ese oi o he wo in ensi e sampling campaigns, ha we e in ag eemen wi h he measu emen s. I was necessa y, howe e , o use a la ge alue o he di usion coe icien du ing he summe mon hs. A 2D model o he elease a ea was de eloped o s udy he beha iou o i ium nea he ANPP discha ge poin . 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