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<br />HYDRAULIC ENGINEERING '94
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<br />Table I, Radio-b'aCked sediment particle parameterS and navel distances.
<br /> Final Fmal Travel Tune Travel
<br />Rock II B~axis Volume Mass SpGr Distance Duration Ve\ocily
<br /> (mm) (mI) (g) (10) (min) (mImin)
<br />10 72 204 502 2.46 732 180 4,1
<br />12 76 213 547 2.57 1065 270 3,9
<br />13 84 242 593 2.45 m 200 . 5,0
<br />14 71 232 601 2,59 686 170 4,0
<br />15 80 235 602 2.56 796 185 4,3
<br />16 76 278 718 2.58 713 175 4.1
<br />17 86 303 728 2.40 347 215 1.6
<br />18 82 299 763 2,55 357 125 2,9
<br />19 77 312 803 2.57 562 160 3,5
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<br />signal to indicate whether the particle is at test or in motion, These particles, rocks 12
<br />and 17, tefem:d to as the momtored rocks, were monitored continuously and the
<br />duration of the test and motion periods wete recorded, The motion sensors used in
<br />this study were built with a delay of 5 s, with the tesult that only test periods
<br />exceeding 5 s were detected, Motion periods of less than 5 s were detected if foUOW<<!
<br />by a detectable test period. Motion periods of 1 s or more were used in the analysis.
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<br />The radio. implanted rocks were placed in the stream at mid-channel. The initial
<br />motion period of the monitored rocks was not included in the analysis; however, after
<br />the first movement they were assumed to have become part of the natural movable boI.
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<br />Shvly Site
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<br />Phelan Creek is a glacier-fed river located on the north side of the Alaskan Rang'
<br />in Interior Alaska, The study site was located approximately 1.6 Ian downstream of
<br />the tenninus of Gulkana Glacier, at an elevation of 1125 m. The drainage area is 31
<br />lan2, of which 70% is glaciated, This study was conducted on 17 August 1990 at a
<br />discharge of 16 m3s- J, near the annual peak, Continuous monitoring lasted about 2
<br />hr, while sediment b'aCking lasted about 4 hr, The entire tracking period took place OIl
<br />the rising limb of the diurnal hydrograph. About midway through the monitoring
<br />period, mean velocity for the stream cross section was 1.93 10 s-1 with a maximwn
<br />mean (in a venical) velocity of 2,82 10 s-I at a total depth of 0.73 10,
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<br />The study reach was about 1000 10 in length with an average gradient ofO.OS
<br />milO, The size of the tracked rocks (b-axis diameter hetween 66 and 86 mm, Tabk
<br />I), falls hetween the D50 and D65 of the bed material as determined by the pebble
<br />count method (Wolman, 1954) on a shon reach within the study reach. At the time of
<br />the study, the stream was capable of easily transporting material in this size range; in
<br />fact, much larger material was in transpon, as evidenced by the sound of boulders
<br />frequently heard roUing in the stream. The data collected in this study are intended 10
<br />show the characteristics of movemeDl of coarse bedload in the size range well below
<br />the maximum size the stream is capable of transporting,
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<br />&mIu
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<br />Describing sediment transpon as a setics of motion and rest periods of the
<br />individual sediment particles was proposed by Einstein (1950), Ergenzinger and
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<br />MONITORING GRAVEL MOVEMENT
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<br />Schmidt (1990), using a radio tracking tecbuique, made the fim Ii ld
<br />''''p length, distance lraveled during the motion period, and n: t e.od ~ts of
<br />lhi, study, we utilized the motion sensor installed with the ~ pen , 1II1ll1on, In
<br />measure 18 and 29 pairs of motion and rest ' ods ~ th tran~tters to
<br />IINo-hour monitoring period. The length of:tion or, e two mOllltored rocks over a
<br />bolh rocks, although most were less tlUIO 20 s In =ods ran14 fium 110 190 s for
<br />periuds :o'ere variable and a single, long resl ~ acco:;.~ ~ e engthhalfs of n:sl
<br />monllonng bme The actual pen:enta f . or over the IOtal
<br />forrockl7 and i7,1% for rack 12 ,eodis~ll1ebuthl1O,enrockof s W~lnand' motion Was 4,3%
<br />L..' era! th .. ' u, motJon resl periods 'ed
<br />~I, In gen ,e majortly of the motion periods OCC'_.' di' , van
<br />,^" IS ted by , ~'OU 10 SbllCl epIsodes of
<br />n~on even . sel"l1'!' relaovely long rest periods (Fi I) Abou '
<br />lhe total Orne 10 mooon of rock 17 OCCIIITed in one ' g, 'sode,' ! two-thirds of
<br />movement o( rock 12 occlllTed in four distinct e ' monoo epl while the.
<br />vanable length (Fig, 1), These data suggesl truJ'~:gr~condiby ~st periodlha s of
<br />easoly transpun the material size once the rocks ' , v), twns t could
<br />10 motion (or e,reoded Il1Otion ePisodes, were pUI m monon they tended to stay
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<br />Rock '17
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<br />2000 4000 C5000 1000 0 0
<br />TOTAL SAMPLING 11MB (s) ~ 4000 6000 aooo
<br />F' ,v,ALSAMPUNG 11MI!~)
<br />19ore 1. Penods of motion and rest for monitored k
<br />roc s.
<br />Travel distances were measured twice tl
<br />,he moniloring period crable 2) Th arrock 12 and ~ for rock 17 during
<br />10 " '. The average ",,"spun v~loci e a~erage ",,"sport velOClnes were 0,36 and 0.50
<br />."'on episodes and 0 5110 s-1 for Iy 0 rock!2 was 0.25 10 s-I after the fll'St three
<br />kknlical to lhat of rock 17, where ~ ~:fu!'I~ (Fig" I), The lalle~ value is nearly
<br />l:'Jl1sodc. The b'anSport velocities nl()(t()n penods occtuTed m one motion
<br />measured by Schmid. and Ergen';;~~) Phe: Oeek are ~parable to those
<br />\-c1ncilies of 0.50 m 5-1 Th .' w reponed maxunum transpon
<br />_imum average wa~ vel~:=';:':d"Y of26~,50fm s-I was 18% of the
<br />\'c1ocuy. or -/0 0 the average cross-sectional
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<br />'n Ihis slOOy, only mean ste length
<br />''''<I distances, the rocks had.Jill s were measured crable 2), For similar
<br />.'"mes the grain diamerer c~ % mean step Ieng!hs of 5,9 and 7,8 Ill, or 77 and
<br />by hostein (1950). Howe~er in a~O- e ~a1ue ,!f 100 IIlIlCS the grain diameter asSUmed
<br />Ilcp' for a mean step length of 84,3 10 IUJ~ pen~ rock 12l1'!'veJ.ed 253 10 in three
<br />In. mean step length of 13,7 10 or 181d II~ tuneS.the.gnnn diameter, Thisresulted
<br />'ho", "'JlOl1ed by Schmidt and Ergenzin;;:(I99!J:'" diameter, values similar to
<br />The distribution of the d ti '
<br />f/t,juc:ncy of shon duration resrura "." of ~t penods is '!ig~y skewed with a high
<br />In upooential function (Einste:,mo:s (yFtg, 2). The distribunon can he described by
<br />, ,angandSayre, 1971), ThePheIanCreei<
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