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and afterward:
Q
h
i
u 0 ¼
(28)
1 þe 1
1 þe 2
HB 1 þ
B 2
The aim of this chapter is to define the river banks influence on tachoida at the
meridian. We have:
3
2
y 1
B 1 þ
ln y 1
B 1
u x y 1 ;
ð
z
Þ¼u 01
1
þ
2
e 1
3
2
z
H þ
ln z
H
e 3
1
þ
2
(29)
and putting y 1 ¼
B 1 we get:
2
Q
BH
ð
1
þ e 1
Þ
ð
1
þ e 2
Þ
3
2
z
H þ
ln z
H
u x z
ð
;
B 1
Þ¼
Þ
1
þ
e 3
(30)
B 1
B 2
B
ð
1
þ e 2
Þþ
B
ð
1
þ e 1
Similar relationships will be obtained when area (2) is considered and
y 2 ¼
B 2 is assumed. The terms that appear in formula ( 30 ) have the following
meaning:
Q
BH ¼ u 0
(31)
is the average velocity in the riverbed cross section. In the further analysis, we
implement a coefficient k in the following form:
ð
1
þ e 1
Þ
ð
1
þ e 2
Þ
k
¼
(32)
B B
B B
ð
1
þ e 2
Þþ
ð
1
þ e 1
Þ
k ( z ), if n 1 and n 2 , the Manning roughness
coefficients of the river banks, vary with depth and the cross section is not
rectangular:
In this way, it is possible to obtain k
¼
u x ð
Þ
u 0 ¼
z
3
2
z
H þ
ln z
H
k
ð
z
Þ
1
þ
(33)
n 2 , values of B 1 and B 2 must be first calculated in order to determine the
location of the river meridian. This division will be found on the basis of the
relationship:
If n 1
e 3 = 2
2
4
3
5
0 ; 75
U 2
n 2
ln
B 1
B 2 ¼
e 3 = 2
and B 1 þ
B 2 ¼
B
(34)
U 1
n 1
ln
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