- Apply the given values and solve for D
Thus, He = 4.5 fHb/lb (1.37 J/N); Qu = 500/20 = 25 ft^3 /(s-ft) [2323 L/(s-m)]. Rearrange
Eq. 26 to obtain
&(He -D)= -^- (26«)
Or, D
2
(4.5 -D) = 25
2
/64.4 = 9.705. This cubic equation has two positive roots, D = 1.95
ft (59.436 cm) and D = 3.84 ft (117.043 cm). There are therefore two stages of flow that
accommodate the required discharge with the given energy. [The third root of the equa-
tion is D = -1.29 ft (-39.319 cm), an impossible condition.]
- Compute the slope associated with the computed depths
Using Eq. 22, at the lower stage we have D = 1.95 ft (59.436 cm); A = 20(1.95) = 39.0 ft
2
(36,231.0 cm^2 ); WP = 20 + 2(1.95) = 23.9 ft (728.47 cm); R = 39.0/23.9 = 1.63 ft (49.682
cm); V= 25/1.95 = 12.8 ft/s (390.14 cm/s); s = [«F/(1.486tf2/3)]^2 = (0.013 x 12.8/1.486 x
1.63^273 )^2 = 0.00654.
At the upper stage D = 3.84 ft (117.043 cm); A = 20(3.84) = 76.8 ft
2
(71,347.2 cm
2
);
WP = 20 + 2(3.84) = 27.68 ft (843.686 cm); R = 76.8/27.68 = 2.77 ft (84.430 cm); V =
25/3.84 = 6.51 ft/s (198.4 cm/s); s = [0.013 x 6.517(1.486 x 2.77
2/3
)]
2
= 0.000834. This
constitutes the solution to part a.
- Plot the D-QU curve
For part b, consider He as remaining constant at 4.5 ft-lb/lb (1.37 J/N) while Qu varies.
Plot the D-QU curve as shown in Fig. 1 Ia. The depth that provides the maximum potential
discharge is called the critical depth with respect to the given specific energy.
5. Differentiate Eq. 26 to find the critical depth; then
evaluate QUetnax
Differentiating Eq. 26 and setting dQJdD = O yield
Critical depth Dc =
2
AHe (27)
Qu= Unit discharge, L/(s»m) H 6 = Specific energy, J/N
(a) Diagram for H 6 = 4.5ft (1.4m) (b) Diagram for Qu = 25 ft^3 /(s»ft)
[2323 L/(s-m)]
FIGURE 11
H 6 = Specific energy, ft • Ib/lb
Critical depth
Qu = Unit discharge, ft
3
/(s«ft)
Critical depth
D =
Depth,
ft
D =
Depth,
m
D =
Depth,
ft