The 50° triangular channel in Fig. E10.6 has a flow rate Q = 16 m^3/s. Compute (a) y_c, (b) V_c, and (c) S_c if n = 0.018.
The 50° triangular channel in Fig. E10.6 has a flow rate Q = 16 m^3/s. Compute (a) y_c, (b) V_c, and (c) S_c if n = 0.018.
Part (a)
This is an easy cross section because all geometric quantities can be written directly in terms of depth y:
P = 2y csc 50° A = y^2 cot 50°
R_h = \frac{1}{2}y \cos 50^{\circ} b_0 = 2y \cot 50^{\circ} (1)
The critical flow condition satisfies Eq. (10.37a):
A_c = \left(\frac{b_0Q^2}{g}\right)^{1/3} (10.37a)
gA^3_c = b_0Q^2or g(y^2_c \cot 50^{\circ})^3 = (2y_c \cot 50^{\circ})Q^2
y_c = \left(\frac{2Q^2}{g \cot^2 50^{\circ}}\right)^{1/5} = \left[\frac{2(16)^2}{9.81(0.839)^2}\right]^{1/5} = 2.37 mPart (b)
With y_c known, from Eqs. (1) we compute P_c = 6.18 m, R_{hc} = 0.760 m, A_c = 4.70 m^2, and b_{0c} = 3.97 m. The critical velocity from Eq. (10.37b) is
V_c = \frac{Q}{A_c} = \left(\frac{gA_c}{b_0}\right)^{1/2} (10.37b)
V_c = \frac{Q}{A_c} = \frac{16 m^3/s}{4.70 m^2} = 3.41 m/sPart (c)
With n = 0.018, we compute from Eq. (10.38) a critical slope:
S_c = \frac{n^2gA_c}{\alpha^2 b_0 R^{4/3}_{hc}} = \frac{n^2 V^2_c}{\alpha^2 R_{hc}^{4/3}} = \frac{n^2g}{\alpha^2 R^{1/3}_{hc}} \frac{P}{b_0} = \frac{f}{8} \frac{P}{b_0} (10.38)
S_c = \frac{gn^2P}{\alpha^2 R^{1/3}_h b_0} = \frac{9.81(0.018)^2(6.18)}{1.0(0.760)^{1/3}(3.97)} = 0.00542