Environmental Engineering Reference
In-Depth Information
Table 5.1 Average monthly sediment concentration and maximum-recorded sediment concentration of ten main
tributaries of the Yellow River
Period of
record
Annual
load (10 6 t)
River
Gauging station
Statistic
June
July
August
Sept
S av
411
523
369
216
64.1
Huangfuchuan
Huangfu
1953-1979
S max
1,370
1,570
1,480
1,240
S av
327
410
373
178
27.8
Gushanchuan
Gaoshiya
1953-1979
S max
1,300
1,190
1,090
829
S av
162
405
319
90.6
135
Kuye
Wenjiachuan
1953-1979
S max
1,400
1,700
1,500
970
S av
12.5
352
323
90.8
106
Wuding
Baijiachuan
1956-1979
S max
1,290
1,270
1,180
958
S av
384
503
448
105
45.3
Qingjian
Yanchuan
1954-1979
S max
1,150
1,080
970
881
S av
287
454
368
119
54.6
Yanshui
Ganguyi
1952-1979
S max
1,200
1,190
1,033
1,070
S av
19
43
59.4
37.6
43.8
Fenhe
Hejin
1943-1979
S max
174
386
227
143
S av
37.1
71.4
80.2
28.5
168
Weihe
Xianyang
1934-1979
S max
654
588
729
662
S av
168
349
329
110
286
Jinghe
Zhangjiashan
1931-1979
S max
906
1,430
984
946
S av
121
337
287
58.1
96.8
North Luohe Zhuangtou 1933-1979 S max 987 1,150 1,190 1,340
S av average monthly sediment concentration in kg/m 3 ; S max maximum recorded sediment concentration in that
month in kg/m 3
A hyperconcentrated flow is non-Newtonian if the sediment consists of a certain amount of clay
particles. The rheological curve of the hyperconcentrated flow approximately follows the following
constitution equation (Bingham model):
d
d
u
y
WWK
(5.53)
B
where W is the yield stress, and K is the rigidity coefficient.
Fine sediment in the flow can be supported by the yield stress and transported for long distance
without deposition and exchange with the bed material. In such a case the concept of “sediment-carrying
capacity” is meaningless. The amount of sediment transported by the flow depends only on the incoming
sediment amount and boundary resistance. Dynamic characteristics of the flow depend on the rheological
properties of the mixture, which in turn depend on the content of clay and silt.
Hyperconcentrated flow is often laminar because of its high viscosity. In the upper central part of an
open channel flow where the shear stress is less than the yield stress, there is no velocity gradient. The
mixture there moves entirely at a uniform velocity u p and forms a flow plug. In wide and shallow rivers
the velocity of the plug u p and the plug zone are given by
2
§
·
J
J
W
W
u
m
h
B
,
h
B
y
h
(5.54)
¨
¸
p
2
K
J
J
J
J
©
¹
m
m
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