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<br /> <br />1686 <br /> <br />(1) <br />0.2053 <br />0.347 <br />0.347 <br />0.347 <br />0.4828 <br />0.4828 <br />0.4~28 <br />0.5056 <br />0.5056 <br />0.5056 <br />0.5246' <br />0.5246" <br />0.5246" <br />0.52461> <br />0.52461> <br />0.5246' <br />0.5409 <br />0.5409 <br />0.5409 <br />0.5861 <br />0.5861 <br />0.5861 <br />4.0769 <br />4.0769 <br />4.0769 <br /> <br />OCTOBER 1973 <br />TABLE 1.-Continued <br /> <br />(2) <br />0.0020 <br />0.0010 <br />0.0015 <br />0.0020 <br />0.0010 <br />0.0015 <br />0.0020 <br />0.0010 <br />0.0015 <br />0.0020 <br />0.0010 <br />0.0015 <br />0.0020 <br />0.00 10 <br />0.0015 <br />0.0020 <br />0.0010 <br />0.0015 <br />0.0020 <br />0.0010 <br />0.0015 <br />0.0020 <br />0.0030 <br />0.0040 <br />0.0045 <br /> <br />(31 <br />2.62 <br />5.41 <br />5.08 <br />6.27 <br />7.60 <br />7.42 <br />7.55 <br />8.17 <br />8.08 <br />8.84 <br />8.31 <br />9.34 <br />8.76 <br />10.05 <br />9.38 <br />9.89 <br />11.34 <br />11.92 <br />12.30 <br />12.11 <br />11.06 <br />11.54 <br />184.18 <br />188.38 <br />195.25 <br /> <br />(4) <br />8.060 <br />5.905 <br />5.038 <br />5.261 <br />4.044 <br />3.918 <br />3.637 <br />3.957 <br />3.644 <br />4.130 <br />3.828 <br />3.314 <br />3.552 <br />3.308 <br />3.232 <br />2.907 <br />3.275 <br />3.114 <br />3.014 <br />3.610 <br />2.990 <br />2.990 <br />1.852 <br />1.746 <br />1.814 <br /> <br />KChanncl width = 2.313 ft (70.5 em). <br />bChnnncl width = 2.416 ft (73.64 em). <br /> <br />Gilbert's "several grains moving" (6), Kramer's "weak movement" (13), U.S, <br />Waterways Experiment Station's "weak movement" (27), and Yanoni's "critical <br />movement" (31). the average velocity was not published by Tison; rather, it <br />was computed by using his Eqs. 4 or 6. When more than one observation <br />was made under similar flow and sediment conditions, the average value is <br />used in the analysis. These data are summarized in Table 1 and plotted on <br />Fig.3. <br />As shown in Fig. 3, when the shear velocity Reynolds number is smaller <br />than 70, the data follow thc hypcrbola <br /> <br />v" <br /> <br />w <br /> <br />HY10 <br /> <br />INCIPIENT MOTION <br /> <br />(51 <br />1 <br />1 <br />1 <br />I <br />3 <br />2 <br />4 <br />3 <br />1 <br />3 <br />2 <br />3 <br />3 <br />2 <br />2 <br />2 <br />2 <br />3 <br />3 <br />5 <br />2 <br />2 <br />3 <br />3 <br />4 <br /> <br />'"I -~-TrITTT-------r III <br />I <br />"I <br />"I- <br />I <br /> <br />I I III r---T-'T--rnl <br />"",.....,,,. <br />,,,., <br />'om".b".,,,, <br /> <br />""'" 1 <br />lL,," <br />""'"' <br />'.""''''''',,'''m'.' <br />''',""0 -- <br /> <br />l <br />i <br />..J <br /> <br />-~-1 <br />1 <br />-1 <br /> <br />t' <br />.) <br />~ <br />~ <br />n <br />l' <br />-1:$ <br /> <br />,,'>- <br />i <br />i <br />,,,1_... <br /> <br />~~'I . <br /> <br />,,,,",,,. -+----~T...."Tr.)N <br />, <br />, <br />, <br />, <br />, <br />I <br />'[' ~:, i <br />L. I <br />,- I ~$(. ('-:!.-'~~;;-,"" ---1 <br />I I ""~~.--'---- I ',,"0": <br />,__ f,,, .,~ ": ' -, "..l...-..~ <br />I . <br />n___L.....LL1.1illL_--L_L.Llllm .L .L, llJJli <br />, '" I~ <br /> <br /> <br />~il" '''0'''' "".Jlb\ ,,,,,,roo '" . ":' <br /> <br />FIG. 3.-Relationship Between Dimensionless Critical Velocity and Shear Velocity <br />Reynolds Number at Incipient Motion <br /> <br />; w4 <br />, <br /> <br />2.Qlut,., (,!lij L!l'i!'i'~ nAIA <br />.,TRAIGHlrllll/llif.l I /" <br />~M!ANLJHINGTH^LW(G ~- <br />4BAAIOln WMlUll ,- <br />/.".Ii. _ <br />/' <br />" <br /> <br />~"y <br />/' <br /> <br /> <br />~ 10) <br /> <br />2.5 <br /> <br />(U,d) <br />log ---;;- - 0.06 <br /> <br />+ 0.66, <br /> <br />U.d <br />o < - < 70 . . . . , . . . . . . , (18) <br />v <br /> <br />~: I~< III') IP" 1<),1 <br />''''L1IH IINIT \1I'rM rOWlfl, v'._v 1'\' I~ Ilm-r":II'." "I~ rDlFN~ rF. "(["'11 <br /> <br />fairly weB, as they should in accordance with Eq. 15. The correlation coefficient <br />and standard error of estimate between observations and Eq. 18 are 0.955 and <br />0.513, respectively. The coefficients used in Eq. 18 were determined by trial <br />and error to minimize the deviation between the observed and predicted values. <br />When the shear velocity Reynolds number is greater than 70, V c;r/ w is no longer <br /> <br />FIG. 4.-Relationship Between Total Sediment Concentration and Effective Unit <br />Stream Power During Process of Channel Pattern Development From Straight to <br />Meandering, and To Braided <br />