Derive the expression for depth of flow in a channel of circular section for maximum flow.
Refer figure.
Let the flow depth be y, and Let the angle subtended be θ.
Wetted perimeter P = 2 R θ
Flow area =(2\ \theta/2\ \pi)\ \pi R^{2}-R\ \sin\theta\ R\ \mathrm{cos}\ \theta=R^{2}\theta-(R^{2}/2)\ \sin\ 2\theta
=(R^{2}/2)\ (2\theta -\sin\ 2\theta)
Using Chezy’s equation,
{Q}=A V=A C~\sqrt{\frac{A}{P}~S_{b}}\;=C\left[\frac{A^{3}}{P}~S_{b}\right]^{0.5}
Q will be maximum if A³/P is maximum. The condition is determined, using
\left[\frac{d{(A^{3}/P)}}{d\theta}\right]=0\quad i.e.,\quad\frac{P\times3\times A^{2}\ \frac{d A}{d\theta}-A^{3}\ \frac{d P}{d\theta}}{P^{2}}=0
or 3P\ {\cfrac{d A}{d\theta}}=A\,{\cfrac{d P}{d\theta}}
P=2\;R\;\theta,\;\;\;\;∴\;\;\;\frac{d P}{d\theta}=2\;R, \\ A=\left(R^{2}/2\right)\left[2\theta-\sin\,2\theta\right] \\ {\frac{d A}{d\theta}}={\frac{R^{2}}{2}}\ (2-2\cos2\theta), Substituting
3\times\ 2R\theta\ {\frac{R^{2}}{2}}\ (2-2\cos2\theta)={\frac{R^{2}}{2}}\ (2-2\sin2\theta)\ 2 R3\theta(1-\cos2\theta)=[\theta-(\sin2\theta/2)]
2\theta-3\theta\cos2\theta+{\frac{\sin2\theta}{2}}=0This is a transcendental equation to be solved by trial, θ = 2.69 radian or about 154°. (check using radian mode in the calculator)
The area for flow =R^{2}\,\theta-\frac{R^{2}}{2}\,\sin\,2\theta=3.0818\,R^{2}
Perimeter =2 R\theta=\;5.3756\;R\;\;\;\;∴\;\;\;R_{h}=0.5733\;R
Depth of flow =R-R\cos\theta={\mathrm{R}}({\mathrm{1}}-{\mathrm{cos~}}\theta)=1.8988\ R{\mathrm{~or~}}0.9494\,D
Note: This uses Chezy equation:
In case Manning equation is used, then the flow,
Q=\frac{A}{N}\left(\frac{A}{P}\right)^{3/2}\;S_{b}^{\mathrm{~}1/2}=\frac{1}{N}\,\frac{A^{5/2}}{P^{3/2}}\;S_{b}^{\mathrm{~}1/2}
\frac{A^{5/2}}{P^{3/2}}\,~\mathrm{or}\,~~\frac{A^{5}}{P^{3}} should be maximized with θ as independent variable
P^{3}\times5\times A^{4}\,{\frac{d A}{d\theta}}-A^{5}\,3P^{2}\,{\frac{d P}{d\theta}}=0, Substituting,
5P\,{\frac{d A}{d\theta}}-3A\,{\frac{d P}{d\theta}}=0 and Substituting for \frac{d A}{d\theta}\mathrm{~and~}\frac{d P}{d\theta}
5\times\ 2R\theta\ {\frac{R^{2}}{2}}\ (2-2\cos2\theta)=3\ {\frac{R^{2}}{2}}\ (2\theta-\sin2\theta)\times2R \\ 5\theta(2-2\cos2\theta)-3(2\theta-\sin2\theta)=0,\quad{\mathrm{or}}\quad4\theta-10\theta\cos2\theta+3\sin2\theta=0
Solving, θ = 2.5007 radian or 143.28°
In this case depth R-R\ \cos\,\theta=R(1-\cos\,\theta)=1.802\ R\quad{\mathrm{or}}\quad0.901\,D