Hydraulic Jump Calculator

Enter the upstream depth and velocity of a supercritical open-channel flow to find the sequent (downstream) depth, energy loss, and jump classification using the Belanger momentum equation.

Quick Facts

Sequent depth
y₂/y₁ = ½(√(1+8Fr₁²) − 1)
Belanger equation, derived from momentum conservation across the jump.
Froude number
Fr₁ = V₁ / √(g·y₁)
A jump only forms when Fr₁ > 1 (supercritical approach flow).
Energy loss
ΔE = (y₂−y₁)³ / (4y₁y₂)
Head dissipated as turbulence; central to stilling-basin sizing.
Jump types by Fr₁
Undular, weak, oscillating, steady, strong
Steady jumps (Fr₁ 4.5–9) dissipate roughly 45–70% of incoming energy.

Your Results

Calculated
Sequent Depth (y₂)
-
Downstream depth after the jump
Upstream Froude Number
-
Fr₁ = V₁ / √(g·y₁)
Downstream Velocity (V₂)
-
From continuity: V₂ = V₁y₁/y₂
Energy Loss (ΔE)
-
Head dissipated through the jump

Ready

Enter the upstream depth and velocity, then press Calculate.

Formula and Method for the Hydraulic Jump Calculator

A hydraulic jump is a sudden, turbulent rise in water depth that occurs when a fast, shallow (supercritical) open-channel flow is forced to slow down into a slower, deeper (subcritical) flow — for example, just downstream of a sluice gate, spillway apron, or weir. Rather than a smooth transition, the flow forms a standing, breaking wave that dissipates a large fraction of its kinetic energy as turbulence and heat. This calculator applies conservation of momentum (the Belanger equation) to your upstream depth and velocity to find the sequent (downstream) depth, the downstream velocity, the head lost through the jump, and which of the five standard jump types it falls into.

How the calculation works

The starting point is the upstream Froude number, Fr₁ = V₁ / √(g·y₁), which compares the flow speed to the speed of a shallow-water surface wave. A hydraulic jump can only exist when Fr₁ > 1, i.e. the approach flow is supercritical. Applying the momentum equation to a control volume spanning the jump in a horizontal, rectangular, frictionless channel (the "specific force" balance) and simplifying gives the Belanger sequent-depth equation: y₂/y₁ = ½(√(1 + 8Fr₁²) − 1). Because the channel width is constant, continuity gives the downstream velocity directly from the upstream discharge per unit width: V₂ = V₁y₁/y₂. The energy (head) lost across the jump follows from the difference in specific energy before and after: ΔE = (y₂ − y₁)³ / (4y₁y₂). The downstream Froude number, Fr₂ = V₂/√(g·y₂), should come out below 1, confirming the flow really has become subcritical.

Jump classification and common mistakes

  • Jump type depends only on Fr₁: undular (1.0–1.7), weak (1.7–2.5), oscillating (2.5–4.5), steady (4.5–9.0), and strong (>9.0). Steady jumps are the design target for most stilling basins because they dissipate energy efficiently (roughly 45–70%) without the wave action of oscillating jumps.
  • Entering the wrong depth: y₁ must be the upstream (pre-jump, shallow, fast) depth. Entering the downstream depth instead will give a Froude number below 1 and the calculator will report that no jump forms.
  • Forgetting the channel assumption: the Belanger equation assumes a horizontal, prismatic, rectangular channel with negligible boundary friction across the (short) length of the jump — it does not directly apply to sloped, trapezoidal, or circular channels without modification.
  • Mixing unit systems: keep depth and velocity in the same system (metric m and m/s, or US ft and ft/s); the calculator uses g = 9.81 m/s² or g = 32.2 ft/s² to match your selection.

Real-world applications

  • Stilling basins below dam spillways and sluice gates use hydraulic jumps to safely dissipate energy and prevent erosive scour downstream.
  • Canal and irrigation check structures rely on jump behavior to control water levels and measure discharge.
  • Storm-drain and culvert outlets are sized so any jump forms in a protected, armored channel section rather than on an unlined streambed.
  • Open-channel flow measurement flumes (e.g. Parshall flumes) use the transition through critical flow — closely related to jump theory — to relate depth to discharge.

Frequently Asked Questions

What is a hydraulic jump?
A hydraulic jump is the abrupt transition of open-channel flow from supercritical (fast, shallow) to subcritical (slow, deep) conditions. It appears as a turbulent standing wave — for example, just downstream of a sluice gate, spillway, or weir — and converts kinetic energy into turbulence and heat, raising the water surface from the upstream depth y₁ to the sequent depth y₂.
What is the Froude number and why does it matter here?
The Froude number Fr = V / √(g·y) compares flow velocity to the speed of a small surface wave. A hydraulic jump can only form when the upstream Froude number Fr₁ is greater than 1 (supercritical flow); if Fr₁ is 1 or less, the flow is already subcritical and no jump occurs.
What is the Belanger (sequent depth) equation?
The Belanger equation, y₂/y₁ = ½(√(1 + 8Fr₁²) − 1), comes from applying conservation of momentum across the jump in a horizontal rectangular channel. It gives the sequent (downstream) depth y₂ directly from the upstream depth y₁ and upstream Froude number Fr₁, without needing to know the turbulent details inside the jump itself.
How much energy does a hydraulic jump dissipate?
The head loss is ΔE = (y₂ − y₁)³ / (4y₁y₂). Weak jumps (Fr₁ around 1.7–2.5) dissipate very little energy, while steady jumps (Fr₁ approximately 4.5–9) — the type most often designed for in stilling basins — typically dissipate 45–70% of the incoming specific energy.