• Keine Ergebnisse gefunden

On the Mediterranean outßow west of Gibraltar*

N/A
N/A
Protected

Academic year: 2022

Aktie "On the Mediterranean outßow west of Gibraltar* "

Copied!
12
0
0

Wird geladen.... (Jetzt Volltext ansehen)

Volltext

(1)

j ").feteor" Forsch.-Ergcbnisse

I

Reihe A No.16 I Seite 23-34

I

Berlin · Stuttgarr

I

Juli 1975

On the Mediterranean outßow west of Gibraltar*

\\'.-\I.TER ZESK, Institut für .\leere~kunde, Kiel

\\'ith 9 fig-ures and 1 tahh:

Zur Ausbreitung des I\fittelmccrwassers westlich von Gibraltar

Z usa!llllll'Jifasslfl~~

Ausführliche Untersuchungen zum Problem der

\X~'asscrverteilung und -Yermischung des mediter- ranen Ausstromes im Golf yon Cidiz wurden im Frühjahr 1971 wiihn.:nd der "Metcor"-Fahrt 23 durchgeführt. l)ie Bc<ll)achtungscrgebnissc stützen sich hauptS:ichlich auf Ilydrosondenstationen, auf Strom- und Temperaturmessungen yon Ycrankcrten Gcdtcn und auf geologische Untersuchungen von KEsros & Bn.nEHso;..,· ( 1973). Der Lcit- charakter der Hodenmorphologie, der zur Aufspal- tung des .. \usstromes führt (.\L\DELAI:"\1 1970), '\vurde prinzipiell bcstiitigt. \\'enigstens \·ier Kanäle konnten durch BcohKhtungen belegt werden. Für drei YOn diesen wird ein ~chitzwert für die mittlere Aus- strommenge angegeben. Danach werden durch den nördlichen ~chelfnahcn .\usstromkanal 0,40 · 106m3 sec-l transportiert. Der Ilauptausstrom YCr- läßt den Golf nm Cidiz in südwestlicher Richtung.

Die Transportmenge beträgt hier 1,39 ·106m3 sec-1.

Eine \\·eitere .\[enge in IWhe Yon 0,24 ·106m:~ sec-1 erreicht den tiefen Atlantik durch ein Tal zwbchen den ZLI\'Or ncnanntcn .:\usstromkanälcn. In einem station{iren \· crmischungsmodcll wird gezeigt, daB 0,95 ·106m3 scc-1 reines ..\littelmccrwasser Yerdünnt mit 1,97 · 1011 m:I sec' .-\tlantikwasscr den Golf Yon C:ldiz verlassen.

Sulllllla!J'

During "Meteor" crdsc 23 in spring 1971 intcnsi\·e invcstigations of the 0lcditerranean outflow in the Gulf of Cidiz wcrc carricd out. In order to givc a hudgct of thc inflow and outflow numcrous

CTD-stations wcre taken. The obscrvations also included six moared current metcr arrays deployed in thc known outflow channcls. Thc considerations giYcn herc arc bascd mainly on thrcc hydro-

~raphic

scctions, current rncter rccords averagcd over onc month, and geological observations from thc hed forms beneath the :,\fediterranean undcr- currcnt. The rcsults show that the outflow csscn- tiallv is dctermincd br the bathvmetrv of thc arca.

At least four separat~ outflow. chan~cls could bc confirmcd. Thc volumentric transport rates of thrcl' of them wcre calculated. These channels arc the northerlv near shclf branch (0.40 · 10° m3 sec 1 ),

thc main. branch (1.39. 106m3 secl) in southwesterly direction, and an intermediate hranch (0.24 · 106m3 secl) found betwcen hoth. In a static box modcl the progressive mixing of 0.95 · 106 rn3 sec-I

pure ..\leditcrrancan \\'ater with 1.97 ·106m3 scc-1 :\orth ~\tlantic Central \'rarer is demonstrated.

lntroduction

The constant exchangc of .-\tlamic and \lediterrancan

\\'ater masses in thc Strait of Gibraltar has hccn a suhject of scicntific research sincc at least 1661 whcn the Royal Socicty of London appro\·cd an expedition for thc im·cstigation of the currcnt systcm in the Strait (sec DE:\COS 1971).

Du ring the 19th century it bccamc \\'eil acccptcd that the steadr inflow of ..\tlantic \'\'atcr through thc Strait of Gihraltar is babnccJ by eyaporation in the :\leditcrranean :;;ea and by an outflow hencath thc surface inflow. Thc warm and hig:hly salinc undcrcurrent sinks due to its high dcnsity until it rcaches a leYcl of equilihrium in thc .-\tlantic watcr.

"'Contribution numhcr 3497 frnm thc \\1nnJ<; llolc Occ:lnt)grarhic Institution

(2)

:\t this point it begins to ~prcad horizontally and forms the upper decp water of thc :\tlantic Occan with its typical intermediate maxima in tcmpcrature and salinit~··

An on·rall vicw of thc hydrography cast and wcst of thc Strait of Gibraltar was shown by

~CIIOTT (1915, 192H) and has hcen reccntly rcpcatcd with ncw data b~· Sn)\1\IEL ct al. (1973). Roth longitudinal sections through thc Strait dcpict the warm and highly salinc outf!o\V west of thc ~ill as a rclatively thin botturn layer which begins to sprcad horizonrally at approximatcly 1000 m dcpth.

Thc prc~cnt paper dcals with thc Jistrihution of thc .\leditcrranean outflow in thc Gulf of Cidiz.

Thc work is bascd mainly on obscn·ational rc~ults

that \\"l'rc obtaincd during the ;...;rorthcast :\tlantic Expedition of R/V "~letcor" in thc spring of 1971.

Thc complctc Iogisries of thc cruisc havc bccn rcportcd by SIEDI.I·:R (1972) including Station and moaring positions and durations of thc rccords.

Thc CTD instrumcnt uscd is of the ).1ultisor.dc type aml has bccn dcscrihcd h)· hROEBEL (1973).

.:\ cornplctc sct of thc currcnt meter Iogs with timc scrics and amplitudc spcctra has heen released in a

>cparatc papcr (ZE"K 1974).

The distribution of the undercurrent 1n thc Gulf of Cidiz

Thc influencc of thc hathymctry of the Gulf of C:idiz on thc ~fcditcrrancan undcrcurrent is at least as important for thc forma.tion of thc Uppcr Deep Atlantic \\'att:r as thc topography of the Strait of Gibraltar itsclf. Thc rcason for this is thc combincd effcct of thc following factors. The undcrcurrent is rnarkcd by high \'clocity which is strongly orientated by dircct contact with thc sca floor. Thc topo- graphy of thc Gulf of Cidiz can bc dcscribcd as a systcm of ridgcs, canyons, and broad terraccs in the contincntal ~dope. :\s a comequcncc of thc high currcnt spccd thc undcrcurrent is strongly influcnccd hy C.oriolisforce and cntrainmcnt prn- ccsses. The ~loping topography accclcratcs thc out- flow with its highl·r dcnsity rclati\·c to thc sur- rounding North Atlantic Ccntral \'\"'ater.

Intensh·e thcorctical studics on steady overflo\vs with thc ~Icditcrrancan as an cxample werc puhlishcd hy S\IITII (1973). In this work thc ohscr- ,·ations of \l.\DEL\1:\" (1970) on the topographic influcncc on thc outflow wcrc mcd for an intcr- comparison bctwccn mndcl computations, labora- rory cxpcrimcnts ar:J thc physical cxample of the

\Iediterrancan outflow. Thc computations show thc combined influcncc of cntrainrncnt and arnbient stratification lirniting thc dcsccnt of thc outflow ro a dcpth of approxirnatdy 1200 rn.

Thc same subjcct was inn:sti,L;atcd by HEEZE:s- &

JOIIS'-'0:\ (1969) with spccial cmphasis on the inter- acrinn bctwecn thc undcrcurrcnt and thc bottom microphysiography. Our knm\ kd,<.';C of this intcr- action recently was irnpron:d h~ k r·SY0'\0 & BELDER- ..;o:-.~ (1973) who showcd hy mctl ' ()f sidc-scan sonar tcchniquc the tracing of the t !l·rcurrcnt on thc sca floor. From thoc and \'ario· .tdditional sources

(GIE~EL & SEIBOLD 1968; S\\ ' I 1)\\' 1969; ZEXK

1971; T!lORPE 1972, 1973; ft·· '1 H, unpublishcd IGY-data) a rather compktc 1 :rc of thc distti- bution of thc umlercurrcnt in t l !. : ulf of C.idiz can hc obtaincd (Fig. 1 ). ;\fter lc;! its sourcc thc outflow turns northwcstward "hout 35o 50'\\' 06'' 40' ~ and is focused in 11arrow strcam.

Further north thc outflow splits ; cvcral channds.

Onc of thcse follows thc out , of thc Ibcrian contincntal shelf while thc rcst

southwcsteri y and northu-cstcrl 1

Lcss, howc,·er, is known a\-.

distrihution of the total outfl<

channcls. The following oh~cr · a morc dctailed undcrstandin~ 1 ~~

· •ws into scYeral

·: \ ons.

1 thc t]uantitati\·c i :1 thcsc ,·arious

':t !11S can suppl~

1 h~· situation lead- ing to thc outflow cascade witl, '1lll1C guantitatiH' valucs.

The cntrance to the Gulf of ( ·:idiz (Sect on A)

in ordcr to study thc outflo\v at it' cntrancc into the Gulf of Cidiz a hydro~raphic cr<h~ scction (.:\) was carricd out at a region whcrl· t hc undcrcurrcnt could hc expccted to bc undi\ idnl (Fig. 2). Thc obscr\'ations obtaincd includcd, k-:-idc thc stations of Scction A, a monring array (.l·quippcd with two thermistor chains and four currcr;t mctcrs) and repea·

tcd CTD casts during 25 hours .. \n on:rall summar~

of thc currcnt mcter data of all moarings discusscd hcrc h. ~i\'cn in Tablc 1.

Taking the 36.0~~0 isohalinc anti its straight cxtcnsion hctwccn station 94 anJ thc contincntal margin as the boundary hctwccn thc highly saline undcrcurn:nt and thc much Jcs:-; salinc ~orth

Atlantic Ccntral \V'atcr, thc outflow occupics an cstirnatcd cross arca of 5 ·106m~. ,\s onc can sec frorn Fig. 2, this area is markcd hy strong vc.:rtical graJicnts in ~alinity and onc might cxpcct that thc outflow causcs a !arge shcar zone at thc boundarics.

Cnfortunatcly two of four currcnt mctcrs that co\-crcd the profilc wirhin currcnt mctcr array 19 failcd. IIO\n:vcr, with thc remaining information of thc mcan specd from rneters 19 105 anJ 19 102 tagether with thcrmistor chain rccord 19 101 and thc assumption of a motionless layer at thc 500-m·

Ievel in thc arca of thc mooring, onc can cstirnatc an intcgratcd mean ~pccd valuc of 35 cm scc-1.

This cstimatc corrcsponds to an averagc flux through

(3)

On thc 1[cditerrancan outflow west of Gibraltar 25

go

so

Fig. 1. Distributic J!l of thc ).1editerranean undcrcurrent in the Gulf of C::tdiz. Dots and squarcs show the position of monring sitcs and CTD stations, rcspcctivcly.

Table 1 1Ican currcnt and temperature data from the Golf c1f t::'tJiz as obtained during ":-.Icteor"

cruL~e 23. hJr detailcd data information, sec ZrsK (107-l-).

70

w

Abb. 1. Verteilung des 1Jcditcrrancn Unterstromes im

Golf \'On G1diz. Punkte kennzeichnen die Lage der

Strommesser-Verankerungen, Quadrate die der CTD- Stationen.

Tabelle 1 ~littlere Strömungen und Temperaturen aus dem Golf von Cidiz nach ~fcssungcn w;ihrcnd der ":..fcteor''-f"ahrt ~r. 23. Ausfuhrliehe Infor- mationen enth:ilt eine D;.tenzusammenstellung von ZE~K (1974).

Rcf. Location Date Dcpth Clea- Speed St. Dcv. Dircc- Temp. St. Dev,

rance Speed tion Temp.

~0. 'I !. Uottom

(") (W) 1971 m m ern/sec OT 'C

19102 36" 05.4' 06' 48.9' 27. 4.-19. 5. 552 112 13 10 351 12.2 0.19

5 -27. 5. 649 15 68 7 324 13.1 0.15

21101 36'18.1' OT 18.1' 27. 4.-27. 5. 557 313 5 7 11.6 0.48

2 649 221 23 12 281 12.6 0.33

3 752 118 29 11 266 13.0 0.15

4 855 15

so

8 243 13.1 0.08

25101 36' 48.7' 07' 55.6' 29. 4.-26. 5. 456 218 40 7 252 13.5 0.49

2 547 127 39 12 259 13.8 0.15

4 616 58 25 10 259 13.6 0.13

5 659 15 20 9 264 13.5 0.17

20101 36' 10.5' 07'27.1' 28. 4.-27. 5. 697 320 10 6 231 10.7 0.35

3 796 221 12 7 231 11.2 0.35

4 901 116 30 15 229 11.6 0.27

5 1002 15 44 13 236 12.6 0.16

22101 36' 19.0' 07' 46.2' 29. 4. -26. 5. 635 465 13 7 270 12.0 0.49

3 884 216 39 11 272 13.0 0.13

4 984 116 22 12 274 12.8 0.13

5 1085 15 9 9 272 12.6 0.09

23101 36' 28.0' 07' 31.0' 28. 4.-26. 5. 448 212 2 3 11.9 0.24

2 539 121 5 4 325 11.6 0.40

3 592 68 22 7 334 12.5 0.36

4 645 15 36 6 319 13.2 0.19

4 Meteor A, 16

(4)

26

0 lO 20 km

or:~~~~~~~~~~ "

dE"pll'l l6

CmJ

200

,00

600

0 10

Fig. 2. Hydrographie scction A through the 1fcditerra- ncan outflow at its entrance into the Gulf of Ci.diz.

Thc trianglcs (Y) denotc thc IO\vering depth of the CTD instrumcnt. 11ooring no. 19 delivcred two currcnt meter

(V.

T) and two thcrm:stor chain (11 X T) records.

The moorcd tcmpcraturc valucs averagcd over thc record length (sec Table 1) arc shown in the dashcd boxes.

Linear intcrpolation bctwecn Stations was clone automa- tically by computer.

Scction A into thc Gulf of Cidiz of approximatcly T., = 1.75 · 10' m3 sec-1.

Taking thc same mixing modcl bet\vcen pure Mcditcrrancan \\"atcr (~lW) ar thc sill (S,1 =

38.4%,) and Norrh Atlantic Central \\'atcr (NACW, SA = 35.6~~0) as was uscd in an carlier study (ZE~K

1970) onc finds that thc undcrcurrcnt with an avc- ragc salinity of S19 = 37.1%0 at cross section A contains roughly 54% pure MW and 46% NACW.

20 30km

Abb. 2. I lydrographischcr Schnitt A durch das aus- strömende :-.tittc!meerwasser am Eingang zum Golf von Cidiz. Dreiecke (T) kennzeichnen die maxim:-dc Einsatz- tiefe der Hydrosondc. :-.littcls Ver:mkerung 1'\r. 19 konn-

~

ten Registrierungen von zwei Strommessern (V, T) und zwei Thermistorketten (11 >: T) gC\\ onncn werden.

Die über die gesamte Registrierdauer (siehe TabeHe 1) gemittelten Temperaturwerte sind in den Kastchen ange- geben. Zwischen den Stationen wurde mit liilfe eines Rechners linear interpoliert.

Typical cstimatcs for thc nct outflow of pure M\V' in thc Strait lic in thc ordcr of T:-,1 = 1. 106m3 scc-1 (c.g. STo:-.t:-.tEL ct al. 1973). This numbcr corrcsponds to T1

9

= 1 · 106m3 sec- 1. 100/54 = 1.85 ·10• m3 sec' for the location of Scction A. Tbc Uiffcrcnce bctwecn T1g and T19 ' is not surprising sincc the outflow in the Strait shows a \Vidc range of Variation. A rneasurcd valuc is not availablc for the time of obscrvation at Scction A.

(5)

On thc ).[editerrancan outHow wcst of GibrJ.\t.lr 27

45 44

dtotn CmJ

moonng no 25 46 s!t\oOn

" " " ,,

100

~~-l[:--~ -,

--

Fig. 3. Hydrographie ~cction B ~outh of Cape Santa ).Iari:l. Thc graph illustratcs two separatcd highly salinc bottom layers betonging to the shelf and to the intermediate branch of the Mcditcrra.- ncan outflow.

Abb. 3. J lydrogr:!phischcr Schnitt ll süd- lich von Kap S:mt.l .\bri:t.. Zwei getrenn- te salzreiche Bodenschichten sind zu erkennen, die die Kerne des schelfn:~.hen

und des Zwischen-Ausstromarmes von ).Jittelmccrwasscr bilden.

<00

600

deottl CmJ

100

<00

600 0

0

Scction A is situatcd in an arca whcre side-scan sonar studics of KE!'.1YO~ & BELDERSO~ have shown the transition betwccn sand ribbons and sand v:aves indicating thc vcry high spccd of the undercurrcnt. Thc maximum instantancous speed mcasured by moaring 19 at 15 m abovc thc bottarn was 84 cm sec-1 \vhich is lowcr than cxpcctcd. The explanation for this rclativcly low maximum which occurrcd onl

r

once du ring onc month ot rccording can bc givcn by the strong shcar associatcd with the high salinity gradicnt. Thc data show that the instrumcnt lcvcl was above the thin corc laycr.

:r-.luch higher s.pceds immediately ncar thc bottarn were observcd carlier in the sill rcgion of the Strait (LACm!BE et al. 1968) as well as in the outflow valleys leading out of thc Gulf of C:idiz (THORPE 1972). In both cases thc maximum spccd excecded 100 cm sec-1.

Two othcr features of the pattern ot sedimcnta- tion are reHected in Section A. The southwestcrn side of the undercurrent coincides with onc ot the

~

"

20km 5['/,,]

___ "-...____...--

-,"_

_____

,.

v - - - _ " _ _ _ _ _ _

_____ " _____ _

(..;-.__" __ _

c.-~:::::::::===---

A-o-,,....,,.."--"---

depositional ridges pointcd out by KENYO~ &

BELDERSO~. The northeastern counterpart could not bc found in Section A. Tbc remarkablc dilution of thc core layer of thc outflow bctwecn stations 95 and 96 rnay bc cxplained in tcrms of mixing bctween the southward Atlantic countercurrent on thc surface and thc outflow. Although no dircct currcnt measuremcnts ot this contincntal shelf current arc known, thc bottom physiography showing long straight crested sand waves indicates its existence.

The shelf branch (Section B)

Soon after passing Section A the undcrcurrent starts to split into sevcral branches each guided by local topographic fcaturcs (MADELAI" 1970). The most northern branch which originatcs from the north- castern sidc of Scction A follows the upper conti- nental slope in a depth range of approximately 400-600 m. At about 7' 30' W the outflow entcrs a channel which opens widcly onto a terrace south

(6)

80 JO 40' JO 20'

w

JO

36° . . 36°

4 ~· ~

" " \

I I 1 11 ~

-ljh ~

I I

I

v-- I '\

'>._'! : \ _ . ' ..

_ + - - - 1 1 - - - T I I

rr

r

1~ " ·"~ ::~ .. 1 ~:;: .• ,.

·:_~:.~:·~·:.:.~~:;:~~~·:::-

---·::. 23 ·::. ''·> ...

·:. I / ' ·.·.~ :" •::.

,.. ()() "'' ~··

·.~:~',,,0~

',/i·,c ·-;.,

·::: __ .,,,,, .. ,-;-:.

,,.·~· ..:: •. • •• -.~ ~-.• • -~ ~-··':.·,

36olll ~::·:;~f)'\:;.. Soo ~-:):11·~-·>., .. , .. ,.·:,.:~.:,~

I " 1'1

20'

~22 :./'':. ;,::: ,,.::r.,. •"''":.. '..;,t '\:

\ .. ··.;·1 ,... ,(··o ·'r~' ·· ... , .

~-J)2J•\ -Nw,k

c:C • { ' :·:

-'"' fr;'.::~.~/\;~~:::.,:".;.,\:\+---+---r---t:l

,·,.. , ...

sa 0\

111

360

20'

·~

I

"---I

I •",,. '\.

ßOÜ

u--woom

"'a

0 '

360~~==========o6=====~7~0~4~07'. =======l==j==~d~==::~====l=====~~:J'! ~

ßu 7°20'

w 70 360

Fig. 4. Bottom topography at moarings 20-23. Herc the roots of the intermediate and the main branch of the 1lediterranean outflow werc identified.

Abb. 4. Bodentopographie in der ümgcbung von Verankerung 20-23.

Hier konnten dtc Ausgang'>gcbictc Jcs Zwischen- unJ des I laupt- Aussrrnm:lrmes des i\fittdmeenv.l<>SCT~ nacht-,t"Wil·~nl \\Tr,Jcn.

N 00

N

~ z

~

(7)

On the ~Icditcrrancan outflow west of Gibraltar 29

7"]()" w

-01-\Y1971 -02 \ -03 -0.

~

\.2J

--

/~

""?~

2~...-::--~~"21

-5o

..-;

X"JO"

N

fig. 5. D::tily aycogcd currcnt vectors in the core of tbc ;\lcditerranean Outflow.

Data from monrings 20-23 are shown for the time interval .Y.Iay 1 through May 24, 1971. The frames are centered arround 36° 20' N and 07" 30' W. For details com- pare \Vith Tablc 1.

Abb. 5. Täglich gemittelte Stromvektoren in der Kernschicht des Mittelmecraus- stromes. Daten der Verankerungen 20-23 sind dargestellt fur den Zeitraum 1. 1Iai- 24. ::-..rai 1971. Der geographische 1Iittel- punkt der Einzelbilder liegt bei 36° 20' N und 07° 30' \\1, \\'eitere Erklärungen sind Tabelle 1 zu entnehmen.

,..

-05

"'

- /

/

"""-

-~ /

- 1 3 "

-~ /

_" \.

-~

7

_" \.

- / 7

"

cm/s..;

-06 \ .

~/

7 -~"

-;::::-

_,."

-~

/

_" \

~ ; /

_" \.

- / /

_"

\.

-06 \ .

~/

7

-~

/

_" "' -· "'

-~

/

-~

/

_" "' _,. "'

- /

/ - / ' /

_" \. _" \.

-~

7 -,--;

7

-n \

_,. \.

-~

7 ~ 7

20105, 24H-AV 121104, 24H-AV 122103, 24H-AV 123104, 24H-AV

1002 m 855m 884m 645m

of the shelf slopc of Cape Santa 11aria. Perpcndicular to this outrunning channel lies Section B (Fig. 3).

At station 47 thc bottarn rise indicates the western end of the depositional ridge which lirnits the shclf branch of 1Ieditcrranean water (GmsEL &

SEIBOLD 1968).

The outflow rnainly is concentrated on two regions, onc an thc southern and one on thc northern sidc of the scction. The southern core between stations 49 anJ 51 bclongs to the intermediate branch discussed latcr whilc thc northern part dcscribes the hydrography of thc shclf branch (bctwcen stations 44 and 47). Thc division of Section B also is evident frorn the "\vcak gcostrophic currcnts which bccome

<2 cm scc-1 below 300m bctwecn CTD stations 47 and 48. The different travel history of both branches was dcmonstratcd by KROEBEL (1973) by mcans of diffcrcnces in light attcnuation factors which wcre rncasurcd sirnultaneously with the T/S profilcs.

The shclf branch shows a dual structure that splits it in an upper and in a lower part. The calculation of the effective cross section yields

0.18 · 106 rn2 for the upper and 1.65 · 10' rn2 for the lower corc. In ordcr to calculate the volurnctric transpatt for the upper vein thc rncan geostropic velocity (13 crn sec-') had to be used whilc the integrated specd for thc lowcr core was obtaincd from current meters 25 104 and 25 105 (23 cm scc-1).

The nurnbers yicld thc flux of T25 = 0.40 · 10' rn3 sec-1.

The mean currcnt records as given in Table 1 show a direction parallel to the shclf in all cases rcflccting the constraint by the southward projcc- tion of the shclf near Cape Santa Maria as mcntioned by KE~ON & BELDERSO~. The rnaximum valuc in the rnean vcrtical currcnt profile appears between 450 and 550 rn depth although Section ß shows no evidcnce of high currcnts in this dcpth range.

An cxplanation for this disagrcement might be found in the rnethod of comparing a quasi-synoptic section with a monthly rnean current profilc. At least the temperature record of 25 101 shows thc highcst variance of all records which highlights the problem.

The maxirnum observed speed appcared in 25 102 with 69 crn sec-1.

(8)

30 ZESK

The intermediate branch (Section B)

Thc evidcnce of this outflow channel was alrcady shown in cross section B tagether with thc shclf branch (Fig. 3). Unfortunatcly no individual hydro- graphic scction is availablc at thc sourcc of this branch. According to Figs. 1 and 4 it starts betwcen two ridgcs both at dcpth of

<

600 m. Thc currcnt rccords abtairred from moaring 23 show a perma- nent northwcsterly outflow in thc depth range of Mcditcrrancan \V'ater (Fig. 5). The thickncss of the outflow was obscrvcd to bc approximately 150m (CTD station 161). According to various topogra- phic charts found in literatute (HEEZEN & Jm-I:-.SoN 1969, liEEZEN & liOLLISTER 1971, JI.!ADELAIN 1970, and KENYON & ßELDERSON 1973) and abtairred du ring thc cruisc (Fig. 4) onc cstimatcs 7.5 km, for the width of thc channcl. Thc current data in Tablc 1 givc the mcan outflow spccd: 21 cm scc-1.

\X'ith thcsc numbcrs the volumctric transport by thc intermediate branch is T23 = 0.23 ·106m3 scc-1.

The cffcct of thc intermediate branch on thc sca bcd has bccn shown in a photograph by MELIERES

Fig. 6. Representation of hydrography (CTD station 6) and topography at moor- ing site 21. The core of the warm anJ highly saline 11editerranean outflow is strongly influenccd by thc local topngr:1phy which causes a leftward veering of thc current profile. The triangles (6 )dcnotc averaged temperatures according to Tablc 1.

Abb. 6. Darstellung -..on Hydrographie (Station 6) und Topographie bei V cranke- rung 21. Der Kern des warmen und salz- reichen 1-Iittclmeerausstromes steht unter dem Einfluß der lokalen Topographie.

Diese bewirkt ein linksdrehendes Strom- profil. Die Dreiecke (6) kennzeichnen die gemittelten Temperaturen im Anschluß an Tabelle 1.

ct al. (1970). During their obscrvations a ncar bottarn specd of 40 cm scc-1 was found which is consistcnt with rccord 23 104 (see Tablc 1).

The main branch (Scction C)

This namc was chosen bccausc thc arca undcr considcration transports the largcst part of thc 1-fcditerranean outflow. A reprcsentation of the charactcristic hydrography and topography at the uppcr end of the main outflow branch is shown in Fig. 6. This picture combincs thc mcan thrcc dimen- sional currcnt profilc (mooring 21) with a singlc T and S-profile (CTD station 6). As thc mcan tempc- raturc values observcd by thc currcnt metcrs indi- catc, thc T-profile displaycd hcre is rather typical for thc location. Deviations bctwccn the continuous profile and thc mcan tempcraturc profilc appcar only at thc depth of the uppcrmost currcnt mctcr (557 m) where the intcrface occasionally passcd the sensor causing thc high ternperaturc variancc of 21 101 (Tablc 1).

(9)

On the 11editerranean outflow west of Gibtaltar 31

moo""ll no 22

66 stat,cn 65 64 moor "'II no 10

62 B2 8t BO 79 ?B 77

'""r~~~======---c=:::::==~=:::::::::::=~=~~

CmJ ~ 63

200

~ c •lil~

- - - J - - - .

@mu 01 Qtoostropl1..: curreont ptof1IP

s

['J .. J

..

CmJ I

"":r=· " 200~~ -=---~"J----"--r---

~"

_____ _ - - · · - - - 1 - - - -

400

_ _ _ _ _ _

"---t~---

- - - -.. - - - + - - - - -

600

600

1000

20 -~

Fig. 7. 1Iydrogr:1phic section C through the m~n-.outflow branch of the :\fcditerrancan outflow and positioos of moaring sitcs 20 and 22. A time shift of 2.25 da)rS-_is indicated by the gap between stations 62 and 82. Maxima of the calculated geostrophic currents are sh0'\\"0 by (:M). Vertically integrated speed values of the outflow are given under thc salinity profile.

Finally from Figs. 4 and 6 thc strong influence of the bottarn topography on thc outflow layer can bc derivcd. Tbc ridges found in the N\V-square of Fig. 6 constrain the fast-flowing near-bottom corc (Fig. 5) to bc dcf!ectcd more southward than

30 40 km

T [°C]

Abb. 7. Hydrographischer Schnitt C durch den Haupt- ausstromaern des }.littelmeerwassers zusammen mit den Verankerungspositionen 20 und 22. Eine Zeitverschiebung von 2,25 Tagen ist durch die Lücke zwischen den Stationen 62 und 82 angedeutet. Zur Kennzeichnung der 1\Iaxima der geostrophischen Ströme wurde das Symbol , (11) verwendet. Vertikal integrierte Geschwindigkeits-

beträge des Ausstroms sind unterhalb des Salzgehalt- s\nittcs eingetragen.

the intermediate and upper layer of the outflow leading to thc leftward veering of the current profile as observed.

Section C in Fig. 7 presents the situation at the lower branch of the main outflow tagether with

(10)

32

depth (m) 200

"0

600

,.,

(!]

t-~~~~~--'---"-

eoo

1000

10

Fig. 8. CTD st:uions 65 J.nJ 78 tngcthcr with ehe gcostrophic currcnt pro!ilc bctwccn Station 6-t and (JS.

The shnwn ::~xeragcd ~pccd and tcmpcraturc Yalues ( .6.) ( moarings 22 :tnd 20) wcrc obtaincd 12 hours prior to the aJjaccnt hydro,C:Llphic stations. Thc graph illustr.1tcs how the outflow cnrc h:~s alrc:tdv lcft thc bnttom at sution 65, while it sti!l toucl~c<; thc bottom at st.ltion 78 (mmp;uc with hg. 7).

360 36.5 SC"/,,J 370 15 TC°C) STATION 713

Abb. 8. I Iydrosondcnst.Hinncn 65 und iK ;;~J".Illltncn mit dem genstrophischen Strnmprofil Z\\ i~clu:n ,kn :-; tatinnen 64 und 65. Die d.lrgcstclltcn c;c.;;dw.·in,li,:~cits- und Temperatur\\ crte (

tJ

aus den Y cr·.mkcrun.c.'l'I1 22 und 20 wurden über 12 Stunden !.!cmittclr. SiL· q.nnrncn aus dem Zeirinten·all vor den· .\fessungcn :tuf <.kll bcnach- b.lrten hydrogr.lphischcn Stationen. I lie I ).lrstdlung zeigt, \\·ie der Kern des .\u.;;-;tromc.;; tkn B,,dcn bei Station 65 bereits Ycrl.lsscn bat, \\ ;d1rcnd er bei Station 78 noch auf dem Boden liegt (\·cr.'-':kichc .\bb. 7).

, - - - . - - - . - - - ,

box model dato sets descnptive terms

n

~

u

n

-

u

pure Med1terranean Wafer

r'"'o'c'---t-'''''~'c--1 ~ r--cm="~'o·'---1

~ ·~

3

r - >-

::l

~k''·

~

~

-

m

_ o 5 C

N m

·· Med1lerranean Outllow"

OBO

117

moor1ng 19 secl•on A moorong 21

moortngs 20,22 (corel,23,25

sect,ons B,C moorJng 22(bottoml

Wust (19361

hydrograph•c th1S paper

s,ource area

Jel-l•ke current

sphll1ng

channels

Fig. 9. Thc outflow cascade of the ..\feditcrranean \X'olter in the Gulf of C1diz.

Abb. 9. Ausstromkaskade des ..\Iittelmcerwassers im Golf von Cldiz.

Heezen a Johnson Kenyon a Beldersan

(19691 119731

rocky

current-swept ~nr.j waves

sechment woves

conyons

smooth topography !arge rT>Jd woves

(11)

On thc .\lcditcrrancan outflow west of (~ibrahar 33 moarings 20 and 22 and thc relative maxima (:\1) of

thc gt.:ostrophic currcnt profiles. The fact that thc data from Scction C \\·ere not obtained simulta- ncously is indicatcd graphically by the gap between station 62 and 82. The cross section ohtaincd shows an uninterruptcd band of outflow water which docs not fit the picturc of two scparatcd outflow channcls for that rcgion as gi,·cn hy 1\L\UEL:\!"S

(1970).

Thc cvidcncc for an uninterruptcd flow betwecn moaring arrays 22 and 20 is consistcnt with

KE~Yo:-; & Bu.IHJbo~·s Fig. 19 that shows at 36° 22' ~. 07' 30' \\.an outflow filamcnt in bctwecn thc channels di~phyt:d hy ..\lAoELAI"S (1970). Re- garding the fidd of motion a significant differcnce bet\vecn monring ~ites 22 and 20 was obser\'ed.

\'\'hile moorin;.,': 20 togcther with CTD station IH (sec Fig. 8) shm\·l·d the same characteristics as moaring 19, i.c. nuximum specd ncar the bottom, thc outflow corc lns lost contact with the bottarn in thc rcgion of monring 22. :\t moaring 20 the highest avcra)-!;t: ~rccd of 50 cm sec-1 was found at 1002 m near thc bottarn whilc thc measured profilc at 22 which fi1 s thc geostrophic calculation (Pig. 8) yiclds a maximum yaJue of 39 cm sec-!

at approximatcly KOO m. As avcragc inten·alls thc 12 hours prior to thc affiliatcd CTD Stations were chosen. In comparing thc gcostrophic currcnt pro- file with thc din.:ctl~· mcasurcd data a positive

\'ertical corrcction of HO m was ncccssary due to thc morc downstrcam rosition of monring 22.

Similar to thc prcvious calculatinn an estimate of the volumctric tramport through Section C was carried out with thc rcsult of T :?Q.:2:! = 1.39 · 106m3 sec-I. Thc calculation was clone under the assumption that all thc outflow of ~lcditcrranean

\~'ater is pcrpcnJicular to thc section. Thc obtaincd valucs of the vcrtically intq!;ratcd geostrophic spccd V :\I and thc IncHions of thcir maxima valucs are included in Fig-. 7.

The region nc<H monring 22 has heen inn:sti- gatcd earlier by Tl!oKPF. (1972) who showcd pic- tures of a scdimcnt cloud bclcnv the 1\lcditerrancan corc. This ohscr\'ation tlndcr thc jct-likc outflow (sec Pigs. 5 and 8) is consistcnt with thc low speed amllow tcmperaturc valucs that \\'erc ohtained from mctcr 22 I 05 (9 cm sec l and 12.6

cq.

The variance of spceJ and tcmpcraturc arc rcmarkably low which favours thc crcation of thc large mud waves as rcportcd hy I-..::1·::-..·yo:-.J & Bm.DERso:-;;.

The south canyon brauch

~-\lthough this outflow branch was not inYestigatcd during ".:\Jctcor" cn!isc 23, therc arc scvcral indica- tions for the permanent cxistcncc of a fourth fila-

5 :\ktcor A, 16

mcnt which separates in a southward dircction soon aftcr passing the gateway at Section ~\.

.\t approximately 36" 00' K, 07, 08' \\' thc halhy- mctric chart :-hows a sharp fcaturc that is formcd hy a Ycry stcep canyon. Sonographs by KE:--.yo;..; &

BELDF.RSO:-i indicatc an abnormally high slopc and a canyon width of 1.5-2.0 km. Hydrographie stations closc bcsidc the channel show at thc bottarn ncarly pure NAC\\-. (e.g. Discovcry ~tation 3990,

Ft'GLISlTR, unpublished) sirnilar to uninfluenccd watcr of thc Sargasso Sca in 500 m dcpth (c.g.

Crawford station 231, Ft:GusTER 1960). At thc DiscoYcry station (35 -, 58' ~. OT' 02' \'\'), a salinity of only 35.74~~0 was obscn-cd 25m abO\·c thc hotrom. This is a strong indication of thc jet-likc character of this outflow filamcnt which lcavcs thc surrounding water masscs relatiYely unaffcctcd.

KF"SYO~ & Br·-.LDF.R:'.O:-..: callcd this branch "thc most problcmatic channd" bccause thc gcological fcaturcs show thc mostintensive interaction betwccn the sca floor and thc undcrcurrcnt.

Thc gcological ohscr\'ations confirm thc hydro- graphic surYC)' by ~L\DEL.'\1:-.< (1970) who illustratcd this branch as a narro\V but separate outflow Yein of highly salinc Meditcrrancan \'\/ater.

r-.:o quantitati\'c value for the transport through thc canyon can bc givcn. However, it is surcly onc rcason for he poorly halanced budget of thc total outflow discussed in thc nc-xt paragraph.

Tbe outflow cascade

In ordn to give a hudgct of the outflow of thc Gulf of Cidiz thc sum of the different outlcts has to bc comparcd with T 19 at thc gate wa y scction.

First of all, howc,·er, thc mixing with KAC\\' in thc arca must bt: takcn into account: an estimate of the \Trtical avcragcd salinity profile wcightcd by thc spccd in Scction _A results in a salinity of S19 --=-37.1%o· Similarly, onc gets a salinity of Ss = 36.5~~0 for thc profilcs in Scctions B and C in thc region of thc outflow wherc its horizontal sprcading starts. Thc salinity of water mixed with S19 to yicld S:-; is again SA .=-: 35.6~{,0 Consequcntly, the watcr that passcs Scction ~'1. (1.75 ·106m3 scc-1) as the i-.lcditerrancan undcrcurrent rcpresents 60~;)

of thc product which is mixed with 40~'0 ~AC\\' (1.17·10Gm3sccl) lcadinp; to a transport of Ts = 2.92 · 106m3 sec I lcaYing thc Gulf of Cädiz.

Fig. 9 illustratcs the proccss bctwccn the Strait of Gibraltar and thc outcr cdgc of thc Gulf of Cidiz in tcrms of a box modcl. Thc Yalucs that wcrc obscrYed during the im·cstigation ~lcteor 23 are markcd by (*) . .-\ll other numbers are deriYed from thcse Yalucs. Thc figurc shows how the mixing progresscs in two stcps (outflow cascadc).

(12)

34 ZE:-;K

\\.hilc thc first stcp of the cascade has bccn descrihcd carlicr (~t:ctinn .\), the sccond includcs thc portions in thc ch:l.tlncls inYestigated hcrc, T :!S· T :!3, and T :!O 1 :!:! as components of T ~· The mcasurcd parts sum up to 2.03 · 106m3 scc-1. .\n unLlt'tt:rmincd outlct Tx = 0.89 · lO!i m:l scc-1 hatl to hc addcd to kccp T s in balancc.

T x cannot be ::.upplicd h~· thc small south canyon hranch alone. Bcsidcs thc contribution from this filamcnr of thc outflow, sc\'cral othcr rcasons haYe certainly influcnc<:d thc pnorly halanccd budgct.

~imilar to thc conncction of thc northcrn and thc southcrn part of ~cction C therc might cxist a continuous layer of outflowing \\·ater hctwccn the southcrn end of Scction C and the south canyon hranch. Such a broad cxt<:nsion of Scction C would b.: abk to transport as much as the sum of T :!n. ::!:! anJ T Other possihlc error sourccs arc thc insufficknt knowlcdg-c of spccd and salinity distri- hution, tkdation from orthog-onality bctwccn scc- tions anJ thc mcan currcnt dircctions, and synopsis prohlcms.

Howcyer, a comparison hetwccn a rcccnt studr hy \\'nRTHJ:'\"GTON (1975) and thc results obtaincd herc shows that T~ = 2.9 ·106m3 sec-1 is in thc right ordcr of magnitude. \\'oRTHI:\"GT0:-1 postulatcs a transport of 3.0 · 106m3 sec-1 in the ~lcditcrrancan outflow to kccp the .·\tlantic circulation balanccd.

Refercnccs

DEAco:-.:, \[. (1971): ~cicntists and the Sc.1 1650 1900. -- AcaJ. Press, 445 pp.

h'CLTHFH, !-'. C (1960): Atlamic Occ.1n Atlas of tcmpe- rattm: and s.t!inirv profilcs and data from thc lnternatinn:d Gcophysical Yc:~r of 1957-1958. --

\\"oods J lolc Oceanngr. lost., \\"oods Hole, :\lao;;o;;, Gn::..n, \\". &

r..

SEiaor.n {19M9: St'dimcntcchogramrne

\"om ihen1-marokkanischcn I-.:onrincnt:~lrand. ".\lc- tcor" J."orsch.-Ergehn., C, 1: 53 -75.

IJLFZL~, B. C. & G. L JoH:-.:soN (1969): ".\Iediterrancan t:ndcrcurrent and .\ricrophysiography west of (;i- hraltar. · · Hull. Tost. Occanogr . .\lon:~co 67 (13H2):

95 PP·

I fErn:-.;, B. C & CD. IloLLIS1T.It (1971): Thc f.1cc of rhe dccp. - Oxford L"ni\"Crsity Press, :\"ew York, 659

rr-

KFsYo:-.;, '\".11. & R. II.l3n.m.n~o:-.: (1973): BeJ fnrms of the .\feditcrranean undcrcurrcnt ohsen·ed with side-scan sonar. ~ ~edimentary c;eology 9: 77-99.

KRot.BFL, \\', (1973): Die Kicler .\Jultimcefessnndc. --

".\1 etenr" Forsch.-Ergchn., :\, 12: 53- 67.

LACO\!ßE, li., F . .\LWEL!\.1:\'" &

J. c.

CASCARil (196H):

Rapport sur Ia Campagne ,Cibralur 1' du na\"in:

ocbnngr:1phique Jean Charcot, 7 auil-12 mai 1967.

- c,h. Oe. 20 (2): 101-IOH.

\f..\DEJ..o\1'-:, !-". (1970): Jnflucnce de Lt topographic du fnnd sur l'i-coulcment .\ICditcrranCen entre lc Dctroit dc Cihr.dt.lr ct le Cap S;lint-\'inccnt. - Cah. Oe.

22 (1): 43--61.

.\fu.ti:nF.s, F., \X'. D. KEsTF.ROI·T & Y. LANCELOT (1970):

I-:tudc photographique des fonds du golfe Je Cadis. -- C:ah. Oe. 22 (1): 63-72.

ScHOTT, G. (1915): Die Gewässer des .\[ittelmecrcs. - Ann.llvdrol!:r. Hin. 43 (1): 63-79.

-- (192R): Oie Kasserbcwegungen im Gchiete der Gibral·

tarstraflc.-

.J.

Consei\3 (2): 139-175.

Thc continuation of thc outflow cascadc to a global scalt: was shown hy \\'i"''iT (1936) by mt.'ans nf all aYailablc hydrographic data aftcr thc ".\h:tcor cxpcdition t<J2S-27. He chosc for thc calculation of mi:dng hctwccn ".\lcditcrrancan \\'atcr and .\tlantic

\Yatcr tht.' following initbl \"alucs: Sum :::.: 36.507~

0

and Sn = 34.68~(~0 \\'hilc Swn is equi\"aknt to S)1 as discusscd hcrc, it sccrns today to hc morc rcalistic to usc for thc othcr watcr mass thc Sargasso Sca \\·'atcr (S_.\) rather than in thc \\'cddcl Sca

\\'atcr (Sn)- This corrcction at thc lo\\Tr end of thc mixing linc howc\·er, docs not changc thc relati\"c

~hapc of thc sprcading of ~kdirerrancan \\"atcr in thc .:\tlantic publishcd by \\'i"sr ( 1936) in bis l:ig. XVJ.

Possihlc rcb.ti\·c changes havc htTO predictcd by thc author hirnself for thc casc of ;1 variarion of thc upper end of his mixing linc.

/1 cknrm .Ju(~c II Im I s

Thc cxpcrimcnt at sea and thc data C\"aluarion wcrc supportcd by thc Deutsche Forschungsgcmcinschaft, Bonn-Bad Godcshcrg. I hcncfittcd from discussions with G. Smm.FR and mcmiK·rs of the \\'oods Hole Buoy Group. Illustrations Wt.'rc draftcd h~- .\. FHIES,

and P. S\!11"!1 hclped mc in prcparing thc English translation.

STEDLJ:R, (;. (1972): ~ordost-Atl.uuik-Expedirion 1971.

.,.\feteor" Forsch.-Lrgchn. A, 10: 79 --95.

S\!IrH, P. C (1973): Thc dymmics of bnttom bnundary currcnts in rhe oce,m, Ph. D. thcsis .\liT.'\\l!OI.

STO\T\!FL, II., II. HRYIHS & P. \f.o\:--;CLL~DO!U (1973):

Does thc .\lcdircrrancan outflo\\" come frorn great dcpth? P;lgcoph 105 (4): 879-RH9.

TIIORPF., S. A. (1972): A scdiment cloud helo\\" the .\fcdi- tcrr:mcan outflow. ~~:Hure, l.ond. 239: 326-327.

-- (1973): .-\n clcctromagnctic current mctcr tn measure turbulent f!uctu:uinns ne:u the oce.1n flonr. - Decp- Sca Res. 30: 933--938.

\\'oRTIII:--;(;To:-o;, 1.. \'. (1975): On thc :\"orth .-\tlantic Circul.lti<m. The Johns lf()pkins Oceanngraphic StuUies (in press).

Wi;ST, (). (1936): Schichtung und Zirkulation des ./\tlantischen Ozeans. ~ Lrg. dt. Atl. Lxp., .\letcor 1925-1927, 6 (1), de Gruyter, Bin. u. Ll'ihz.

Zr.r-;K, \\'. (1970): On temper.lturc and salinitv srructure of the .\fediterr:lnean \\'atcr in the :'\orthC.1st Atl:in-

tic. ~ Dccp-Se:1 Res. 17: 627- 632.

-- (1971): Zur Schichtung des :\littclmccrwasscrs \\est- lich Yon (iihrahar. ~ ".\[etcnr" Forsch.-Enrebn. A,

9:1-30. c

(1974): Some current and tempcrature ohscrvations in thc .\tcditcrrancan outf!ow wcst of Gihralt.1r; a data rcport - .,.\lcteor" l"orsch.-Lrgehn. A, 15: 20-4?'1 .

Recei,·ed Juli 5, 1974

Referenzen

ÄHNLICHE DOKUMENTE

Two subsequent measurements of the top quark pair production cross section in the single lepton channel are presented with 35 pb −1 of data and 0.7 fb −1 of data in chapters 6 and

In addition, the fundamental frequency is substantially lowered during laryngealization, and there may be period- to-period irregularities in both the duration of the period

Après avoir pu terminer les travaux analytiques pour déterminer le Tetrahydrocannabinol (THC) dans les aliments contenant du chanvre (voir rapport annuel 1997), il s’est posé

In the next step, it was examined whether significant differences can be found between the THC-set and the CAN- set and between the CAN-set and the DFI-set in the areas under

The cannabinoids in the obtained extract were quantified by LC–MS-MS and used after dilution for further testing of the CR of (–)-trans-THC-COOH-Gluc with a homogenous enzyme

The aim of the pain study was to test the antinociceptive effects of oral THC and THC combined with morphine (THC-morphine) versus morphine and placebo in healthy subjects

Continuous temperature (1) and salinity (S) profilcs from thc North Atlantic often show a doublc- maxima structurc in the ~lediterrancan Outflow (hcnceforth ~!

This paper presents the obtaincd rccorcls of 29 current rneters and 5 thcrmistor cables in thc form of time series, amplitudc spcctra, and progressive ycctor