Skip to main content

94% depth for maximum discharge in circular channel

Short answer

For maximum discharge in a circular channel, differentiate Manning's equation with respect to the angle θ, leading to 5θ(1-cosθ)=2(θ-sinθ). Solving gives θ=302.4°, and depth y = 0.5d(1-cos(θ/2)) ≈ 0.94d, i.e., 94% of the diameter.

Using Manning's equation, show that the depth of flow is equal to 94% of the diameter for the partially filled most economical circular channel considering maximum discharge.

Condition for maximum discharge

Manning: Q=1nAR2/3S1/2=S1/2nA5/3P2/3Q=\dfrac1nAR^{2/3}S^{1/2}=\dfrac{S^{1/2}}{n}\dfrac{A^{5/3}}{P^{2/3}}. For constant dd, nn and SS, QQ is maximum when A5/3P−2/3A^{5/3}P^{-2/3} is maximum:

dQdθ=0  ⇒  5PdAdθ=2AdPdθ\frac{dQ}{d\theta}=0\;\Rightarrow\;5P\frac{dA}{d\theta}=2A\frac{dP}{d\theta}

Geometry

Let θ\theta be the angle (rad) subtended at the centre by the wetted arc:

A=d28(θ−sin⁡θ),P=dθ2,dAdθ=d28(1−cos⁡θ),dPdθ=d2A=\frac{d^2}{8}(\theta-\sin\theta),\quad P=\frac{d\theta}{2},\quad \frac{dA}{d\theta}=\frac{d^2}{8}(1-\cos\theta),\quad\frac{dP}{d\theta}=\frac d2
    ___
  /  |  \     y = depth
 |   |th |    d = diameter
  \  |__/
    ---

Solution

5(dθ2)d28(1−cos⁡θ)=2 d28(θ−sin⁡θ)d25\left(\frac{d\theta}{2}\right)\frac{d^2}{8}(1-\cos\theta)=2\,\frac{d^2}{8}(\theta-\sin\theta)\frac d2 5θ(1−cos⁡θ)=2(θ−sin⁡θ)5\theta(1-\cos\theta)=2(\theta-\sin\theta) 3θ−5θcos⁡θ+2sin⁡θ=03\theta-5\theta\cos\theta+2\sin\theta=0

Solving by trial (or Newton's method): θ=5.2781\theta=5.2781 rad =302.41∘=302.41^\circ.

θ\theta (deg)3θ−5θcos⁡θ+2sin⁡θ3\theta-5\theta\cos\theta+2\sin\theta
2904.649
302.40.000
310-2.690

Depth of flow

y=d2(1−cos⁡θ2)=d2(1−cos⁡151.21∘)=0.9382 dy=\frac d2\left(1-\cos\frac\theta2\right)=\frac d2\left(1-\cos151.21^\circ\right)=0.9382\,d

So the depth for maximum discharge is y≈0.94 dy\approx0.94\,d (94% of the diameter).

✓ Answer checked by Claude Opus 5.5 (high effort)

All Hydraulics chapter 6 questions →