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Hydraulic jump: derivation and numerical

Short answer

Downstream depth is 1.34 m, velocity 1.34 m/s, Froude number 0.37, head loss 0.70 m, and power dissipated 12.4 kW per metre width.

(a) Define hydraulic jump. Derive the relation between the conjugate depths y1y_1 and y2y_2 of a hydraulic jump in a horizontal rectangular channel, and the expression for the head loss. (b) Water flows at 6 m/s with a depth of 0.3 m in a wide horizontal rectangular channel and a hydraulic jump forms. Find the downstream depth and velocity, the downstream Froude number, the head loss, and the power dissipated per metre width.

(a) Hydraulic jump

A hydraulic jump is the sudden rise in water surface when a rapid (supercritical, Fr>1Fr > 1) flow changes to a slow (subcritical, Fr<1Fr < 1) flow. It is a turbulent phenomenon with large energy dissipation.

Derivation (horizontal channel, unit width, neglect friction on the bed): apply the momentum equation to a control volume enclosing the jump.

Hydrostatic forces: F1=12ρgy12F_1 = \tfrac12\rho g y_1^2 and F2=12ρgy22F_2 = \tfrac12\rho g y_2^2. Discharge per unit width: q=V1y1=V2y2q = V_1y_1 = V_2y_2.

12ρgy12−12ρgy22=ρq(V2−V1)\tfrac12\rho g y_1^2 - \tfrac12\rho g y_2^2 = \rho q (V_2 - V_1)

Using V1=q/y1V_1 = q/y_1, V2=q/y2V_2 = q/y_2:

g2(y12−y22)=q2(1y2−1y1)=q2(y1−y2)y1y2\frac{g}{2}(y_1^2 - y_2^2) = q^2\left(\frac{1}{y_2} - \frac{1}{y_1}\right) = \frac{q^2 (y_1 - y_2)}{y_1y_2}

Dividing by (y1−y2)(y_1 - y_2) and rearranging:

q2g=y1y2(y1+y2)2\frac{q^2}{g} = \frac{y_1y_2(y_1 + y_2)}{2}

With q=V1y1q = V_1y_1 and Fr1=V1/gy1Fr_1 = V_1/\sqrt{gy_1}, this gives the quadratic in y2/y1y_2/y_1:

(y2y1)2+y2y1−2Fr12=0⇒y2y1=12(1+8Fr12−1)\left(\frac{y_2}{y_1}\right)^2 + \frac{y_2}{y_1} - 2Fr_1^2 = 0 \quad \Rightarrow \quad \frac{y_2}{y_1} = \frac12\left(\sqrt{1 + 8Fr_1^2} - 1\right)

Head loss: hL=E1−E2h_L = E_1 - E_2, where E=y+V22gE = y + \dfrac{V^2}{2g}. Substituting from above:

hL=(y2−y1)34y1y2h_L = \frac{(y_2 - y_1)^3}{4y_1y_2}

(b) Numerical

Given y1=0.3 my_1 = 0.3\ \text{m}, V1=6 m/sV_1 = 6\ \text{m/s}.

q=0.3×6=1.8 m2/sFr1=69.81×0.3=3.497y2=0.32(1+8(3.497)2−1)=1.341 mV2=qy2=1.81.341=1.342 m/sFr2=1.3429.81×1.341=0.370\begin{aligned} q &= 0.3 \times 6 = 1.8\ \text{m}^2/\text{s} \\ Fr_1 &= \frac{6}{\sqrt{9.81 \times 0.3}} = 3.497 \\ y_2 &= \frac{0.3}{2}\left(\sqrt{1 + 8(3.497)^2} - 1\right) = 1.341\ \text{m} \\ V_2 &= \frac{q}{y_2} = \frac{1.8}{1.341} = 1.342\ \text{m/s} \\ Fr_2 &= \frac{1.342}{\sqrt{9.81 \times 1.341}} = 0.370 \end{aligned}

Head loss and power:

hL=(1.341−0.3)34×0.3×1.341=0.702 mP=ρgqhL=1000×9.81×1.8×0.702=12 390 W/m=12.4 kW per m width\begin{aligned} h_L &= \frac{(1.341 - 0.3)^3}{4 \times 0.3 \times 1.341} = 0.702\ \text{m} \\ P &= \rho g q h_L = 1000 \times 9.81 \times 1.8 \times 0.702 = 12\,390\ \text{W/m} = 12.4\ \text{kW per m width} \end{aligned}

Since Fr2<1Fr_2 < 1, the downstream flow is subcritical, as expected.

Answer: y2=1.34 my_2 = 1.34\ \text{m}, V2=1.34 m/sV_2 = 1.34\ \text{m/s}, Fr2=0.37Fr_2 = 0.37, hL=0.70 mh_L = 0.70\ \text{m}, P=12.4 kW per metre widthP = 12.4\ \text{kW per metre width}

✓ Answer checked by Claude Opus 5.5 (high effort)

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