Technical Report Series Number 77-2 32 r 32 I I I J CHARACTERISTICS OF WATER FLOW AT THE NORTH END OF THE WASSAW BARRIER ISLAND COMPLEX Wassaw Island Erosion Study Part II by George F. Oertel 31 31 Georgia Marine Science Center University System of Georgia Skidaway Island, Georgia 81 CHARACTERISTICS OF WATER FLOW AT THE NORTH END OF THE WASSAW BARRIER ISLAND COMPLEX WASSAW ISLAND EROSION STUDY PART II by George F. Oertel Skidaway Institute of Oceanography P.O. Box 13687 Savannah, Georgia 31406 The Technical Report Series of the Georgia Marine Science Center is issued by the Georgia Sea Grant Program and the Marine Extension Serv i ce of the University of Georgia on Skidaway Island (P.O. Box 13687, Savannah, Georgia 31406). It was established to provide dissemination of technical information and progress reports resulting from marine studies and investigations mainly by staff and faculty of the University System of Georgia. In addition, it is intended for the presentation of techniques and methods, reduced data and general information of interest to industry, local, regional, and state governments and the public. Information contained in these reports is in the public domain. If this prepublication copy is cited, it should be cited as an unpublished manuscript. INTRODUCTION This report supplements an earlier report on the ••sedimentary framework of a channel margin shoal of an ebb delta, Wassaw Sound, Georgia 11 • The purpose of this report is to produce an overview of water currents that may affect the sediment carpet described in the earlier report. Water flow was recorded at four different stations around the marginal shoal (Fig. 1). At each station, data was recorded for two tidal cycles (approximately 25 hours) at six minute intervals. In all, approximately 2,000 data points were collected. OBSERVATIONS Stations A and B were located on the leeward side of the shoal and stations C and D were located on the channelward side of the shoal. Plotted data of water flow surveys illustrate the reversing flow of tidal currents above the shoal and adjacent shoreface. In all cases, flow reverses corresponded to the predicted change in the semi-diurnal tide (Figure 2,3,4,5). Maximum current speeds were recorded at station C located at approximately -6 meters (MLW) on the margin of the shoal and the channel. Station D was located approximately one quarter mile closer to the shoal than station C and at approximately -2 meters (MLW). The mean current speeds at stations C and D were 40 cm/s and 20 cm/s, respectively. Higher velocities at station C illustrate the channel- ized flow of the main channel. Increases in caused a reduction in flow speed. flow of water was the main channel. 11 Shielding 11 11 bed drag at station D 11 During the ebbing tide the offshore by the marginal shoals and confined to During the flooding tide, 11 Shielding caused water 11 Soutl1 Carolina N J .c ~ c. ·----=- --5 10 .,. B• -2m Noull col Milt 5 ~=- Nouli c ot UUes 0 '~,"':>\ • ATLANTIC OCEAN ............_ ...... 0 1/2 20 • slolion loco lion Figure 1. Location map of study area and current meter stations. ·-.... - 2m Meter A May 28, 1975 20 50 80 ,I 'I I I ~ "' Cl) Cl) '01 II 140 , I I \./'""' \ I /I I I ,' \~ ~ I I I I I 170 Cl) 0 4 I 110 200 ,-, I I I ,, I "! , ...·.·.·.·.···········-·.·,·., ' ,.. I 1---\ I ' - : 60 < (1) 40 20 I 0 230 0 3 2 0 ;;;- 0 .;: 260 0 Cl) -~ 0 - '< ::l c c g I 290 320 I, I I I 1 I I I'' I I I .__, '~ I I II. I \ \ \ 350 (1) I r" ,_/ ) I 40 "I _,"''' •..J I! I \~ I I I I _/',1 I ,, ~ \ '/' ,, . \ ~ ......... \ I I I . I , ......... I 1 20 soT ,, I 0 ,, . r 50 2 Figure 2. 4 6 8 10 12 14 Time in Hours 16 18 20 22 24 26 Graphic representation of tidal current velocities and directions at Station A during a 26-hour interval (2 cou1plete tidal cycles). Stippl ed area indicates the portion of the sample when velocities were above the estimated threshol L. velocity for the sediment at the seabed. VJ Meter B June 5, 1975 90 60 -:1/"'\ "' I • tl t II II I It I j I Jl til \ l11l I I 1 11 \ I ,. I I I I I I ,, " I I I • ~ ~ r 4 ~ II I II I II 1/ , 1 1I A I II 11 .4 \ 1I #I 1 1 \1 I I IJ I 1I I \" I I I I ~ I II AI I, I 1 II11f. I /' I I 11 1 \ I I I I ~ I 1 '· ._ .. • • (/J A P• I t II I .......... A ~ II\ I 1.! ~ \ 'I I I - I • I .~ I I I l G> ··""'p;:........_J_ l-40 I I ' ~-,30 ~ 20 Q) ..... 01 10 ::::J 0 c: ---~ 270 0 240 10 ..... 0 3 ........... I u G> - '< G> c g-· I I I I I 0 180 150 I 1 r l '', I 1 2 4 6 ~ II I 1 • ~ U I I • I I I'/ I~I I '· 1~ II 90 .4 I I I II , n I / I( I ' 1 1 It I I I ~ I I 120 20 30-- I I 8 I I I 1 l II J I r 11 r ll 1 II 1 Ill _! ~ I I 10 12 I I I I "-J A '' /d I " I II '·'1:I v 14 16 18 j 20 I /' "~ I I I I ,I I 22 rl I I' 11 I I II I 1I , \ I 111 I I tl tl ' CD 0 T I 210 (/J I 11 II 40 I I ~ uI f 24 26 Time in Hours ""' Figure 3. Graphi c representation of tidal current velocities and directions at Station B during a 26- hour interval (2 complete tidal cycles). Stipp l ed area indicates the portion of the sa111ple when velocities were above the estit»ated threshol d velocity for the sediment at the seabed. ,, \ 90 4> 110 140 c: g- - I :J. . . 1/~ .~:~~j,.:,l I I 0 0 I 1 I ~ C1) I I \ I (/) Q) April 28, 1975 : ,...__ J, c It It 50 -1 I I Meter I 20 -1 g- 40 .·:·:·:·:·:·:·:·:·:·:·:-:·:·:·:·:·:-:·:·:·:·:·:·:·:· -+ 20 '< - :J 200 0 1\ I 230 - ~ _}l II\ 290 I II , - "'' ,.,.... .....I 320i I I r I 350-i 2 4 / I f \' I "I \ I \ - "'' -"" ' 6 /t /\ I \.--" /\~- / \ \/ 8 10 12 14 16 18 20 0 3 ~ 20 :~ ·; ~ 260 '- 0 (1) I I 170 < - (1) 40 I ") 1" I \ v \I I /\1 .......... \J ~ 22 24 26 Time in Hours V1 Figure 4. ° ,-... Graphic representat i on of tida l current vel oc i t i es and directions at Stat i on C during a 26- hour interval (2 comp l ete tida l cyc l es). St i pp l ed area indicates the portion of t he sa111p l e when ve l ocities were above the estinlated threshol d ve locity for the sediment at th e seabed. : \ ,........ 1I 90 1 ....!., 110 a.... 140 Ol Cl) 0 c: I I \ I I (/) C1) C1) April 28. 1975 'I II 50 I I Meter C ,,I 20 .....·.·...... ....~. ~.~,·.·.·. ,- < (1) ~ 170 g 20 '< ..... :l 200 0 0 3 ~ 230 - ..... 260 Cl) 20 I \J 40 ,., I "I ' 290 (1) ' " r -"'' , I 320 ',-'' I 350 2 4 ,.....- " I \ I \..-""' I 1\1 .......... \I \ \-" ' ..... .J 6 " ) t" I \ v \I 0 T I I /I ;n- I ·••... ......-s 0 0 40 ~ 8 10 12 14 16 18 20 22 24 26 Time in Hours lJl Fi gure 4. Graphi c representat i on of t i da l current vel oc i t i es and di rect i ons at Stat i on C during a 26- hour interva l {2 comp l ete tida l cyc l es). St i pp l ed area i ndicates t he portion of t he samp l e when ve l ocit i es were above the est i mated t hres hold ve l ocity for the sed i ment at the seabed. Meter D ,, ~ I I I I June 5, 1975 I I I 40 30 < (J) 20 0 0 - '< ~--~~----~r---~~~~~----~------1~ 10 :l 0 3 ;;,. (J) 0 20 -. IA kI II I t 1 1' I 1 r Ill / II lr 1111 I 11 u ,1,, 30 40 -1 tfJI 11 11 I 4 6 8 10 12 14 16 18 20 22 24 26 Time in Hours 0\ Figure 5. Graphic representation of tidal current velocities and dire ctions at Station D during a 26- hour interval (2 complete tidal cycles). Stippled area indicates the portion of the samp l e when velocities were above the esti111ated threshold velocity for the sediment at the seabed. 7 to flow northeast around the distal end of th e shea l and "spi 11 into the main channel. 11 In the channe l , l andward flo od in g wat er was confined by channel wa l ls and fl0w wa s t o the northwest. Flow vectors were determined at each station by obtaining the products of the mean speed and duration, and plotted in the mean di rections for the ebb and flood. Vectors and the graphic resultants of vectors are illustrated in figure 6. The resultant of the ebb and flood vectors at station 0 was oriented toward the central axis of the channel. The resultant at station C was very sma ll and oriented away from the channel ax i s. After two complete tidal cyc l es, stat io n 0 appeared to il lu strate a residual flow of water "spilling of the main channel. 11 over the shoals toward the axis This was produced by the flow of flood water toward the channel axis and not directly toward the inlet throat . The flow at station C was parallel to the axis of the main channel and directly toward the inlet throat during flood tide and directly away from the inlet throat during ebb tide. Although stations A and B were shie lded from the main channel by marginal shoals, they al so illu st rated semi- diurn al reverses in flow direction. The speeds were 25 cm/s and 19 cm/s fo r stations A and 8, respectively. At station A, the flood vector was oriented toward the end of Wassaw Island, and the ebb vector was oriented in a southeast direction. The resultant of the ebb and flood vectors was oriented toward a 11 spi 11 over 11 channe 1 in the shea 1. Observations indicate that water flows over the entire shoa l surface during the earl flood and is issued through 11 11 Spill-over 11 channels during the l ate flood. The l argest Spi11-over 11 channel on the marginal shoa l was located adjacent to Stat ion A. -2m -2m .uili.._ ...ili... ...uit.._ ~L.. .Jlt... .ulu... ..ill£.__ ..uJu. dlu._ 0 ,o~ ...lili..... \c;_, 0~ ~ c;_, ~oc;_, -2m Nautical Miles ~ 0 I 1/2 Vector Seale 0 Figure 6. 3000m 6000m Vector map for all current velocities recorded lm above the seabed. Vectors are the product of the n~an direction and speed for the ebb and f lood portions of the two canplete tidal cycles. The resultant is the graphic average of the ~b b and flood vectors. 00 9 At station B, water is transported toward the axis of the shoal during the flood, however, ebb currents are southeasterly and parallel to the axial flow of the main channel. The resultant flow at station B was toward the axis of the main channel but in an offshore direction. / The general scheme of circulation is similar to the models pre- sented by Oertel (1974) and Hayes (1975). Reversing tidal currents are the major agents of water transport at Wassaw Inlet. On the inlet side of the shoal reversing tidal currents were bipolar and parallel to the channel axis as a result of confinement by the channel walls. On the leeward side of the shoal, ebbing currents paralleled the axis of the shoal and channel, however, flooding currents were oblique to the axis and flowed toward the channel. The resultant flow from stations outside of the main channel is toward the channel axis and not necessarily toward the inlet throat. While the data described above yields information on the total velocity field, only a portion of these velocities is competent enough for sediment transport. A gross estimate of the sediment-transporting currents is made by plotting the resultant of the duration and mean velocity of currents greater than 25 cm/s (estimated threshold velocity). In figure 7, ebb, flood and resultant vectors were plotted for produtts of the duration and speeds greater than 25 cm/s. The resul- tant vectors representing these currents were considerably smaller than the vectors for the total velocity field. resultant flow was toward the channel axis. Leeward of the shoal, the In the channel (station C) the sediment flow was small and away from the channel axis. The resultant pattern of potentially competent currents is toward the axis of the marginal shoals. Observations of bedform orientations appear to confirm this pattern. On the channelward side of the shoal, -2m - 2m _ill!L _illiJ._ ....ultL._ ...ili.._ ...~~~.__ ...1L. .-DlLL -2 m ..,_\lu..._ ...ili,_ ~ ,(}~ ...illu_ B~ \C:J (}~ ..illkt..... ··. C:J ·~ ~(}C:J -2m Nautical Miles ~- 0 1/2 I Vector Scale 0 Figure 7. 3000m 6000m Vector map for current velocities greater than 25 em/sec recorded lm above the seabed. Vectors are the product of the mean direction and speed of velocities greater than 25 an/sec for the ebb and flood portions of two crnnp lete tida l cyc les. The resultant is the graphic average of the ebb and flood vectors. t-' 0 megaripples appeared to be migrating toward the shoal axis in an oblique offshore direction. On the leeward side of the shoal, megaripples appeared to be migrating toward the shoal axis in an oblique onshore direction. Spill-over channels that transect the shoal surface are important structures necessary for maintaining this type of sand and water circulation. he spill-over channel closest to the shore is particu- larly important for bringing sediment to the north end of Wassaw Island. Events that produce the closure of this channel, would consequently cause stagnation of sediment in the floor of the spill-over channel and decrease the quantity of sediment being transported to the adjacent beach and shoa l . The sediment starved area at the north end of Wassaw would erode until the spill-over channel was reopened. 12 ACKNOWLEDGEMENTS This project was sponsored (in part ) by the Georgia Sea Grant Program, supported by N.O.A.A., Office of Sea Grant, Department of Commerce, under grant no. 04-5-158-4. and distribute reprints for The u. S. Government is authori zed t o produce governmen t a~ purposes not withstanding any copyright notation that may appear hereon. 13 REFERENCES Hayes, M.O., 1975, Morphology of sand accumulations in estuaries, .ill Cronin, L.E. (ed. ), Estuarine Research, 2, Academic Press, New York, N.Y. Hoyt, J.H., R.J. Weimer and V.J. Henry. 1964. Late Pleistocene and Recent sedimentation, central Georgia coast, U.S.A., p. 170176, .l!J. Straaten Van, L.M., J.V. (ed.}, Deltaic and Shallow Marine Deposits, Elsevier, Amsterdam. Oertel, G. F. and C. F. Chamberlain. 1975. Differentia l rates of shoreline advance and retreat of coastal barriers of Chatham and Liberty Counties, Georgia. Trans. Gulf Coast Assoc. Geol. Soc. XXV: 383-390. •