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Water and Hydraulics Structures Branch / 3rd Class [Hydraulic Structures]
Lect.No.4-First Semester [Critical Flow Computations]
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Lect.No.4-First Semester [Critical Flow Computations]
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Water and Hydraulics Structures Branch / 3rd Class [Hydraulic Structures]
Lect.No.4-First Semester [Critical Flow Computations]
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**** For a rectangular channel section of bottom width b, the Froude number is
expressed as;
where, q=Q/b=discharge per unit width and is defined for rectangular channels
only. Then the expression for the critical depth becomes;
…………………… (6)
**** For a triangular channel with side slopes of “m” (that is 1 vertical over m
horizontal), the critical depth calculated as;
…………………… (7)
**** For a trapezoidal channel with side slopes of m (that is 1 vertical over m
horizontal), Fr = Fr2 = 1, will lead to;
……………… (8)
Eq.8 cannot be solved for (yc) explicitly. Therefore, a trial-and-error procedure is
needed to determine the critical depth for trapezoidal channels. Alternatively, can
Figure (T), can be used, which presents a graphical solution for Eq.8 in
dimensionless form.
Water and Hydraulics Structures Branch / 3rd Class [Hydraulic Structures]
Lect.No.4-First Semester [Critical Flow Computations]
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Figure (T)
**** Likewise, for a circular channel of diameter d0, we can show that
(Henderson,1966)
……………… (9)
Where;
An explicit solution to Eq.9 for yc is not available; so it solved by trial and error.
However, a graphical solution is provided in Figure (C) to facilitate the calculation
of the critical depth in circular channels.
Water and Hydraulics Structures Branch / 3rd Class [Hydraulic Structures]
Lect.No.4-First Semester [Critical Flow Computations]
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Figure (C)
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Lect.No.4-First Semester [Critical Flow Computations]
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Lect.No.4-First Semester [Critical Flow Computations]
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Lect.No.4-First Semester [Critical Flow Computations]
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Lect.No.4-First Semester [Critical Flow Computations]
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Lect.No.4-First Semester [Critical Flow Computations]
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Lect.No.4-First Semester [Critical Flow Computations]
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