Rectangular channel
For Q = 100 cfs and b = 10 ft, the direct formula gives yc = 1.46 ft, Vc = 6.85 ft/s, and Emin = 2.19 ft.
Use the critical depth formula for circular, rectangular, trapezoidal, and triangular channels. Calculate critical depth, velocity, minimum specific energy, and Froude number in US customary or metric units.
Quick answer
Critical depth (yc) is the flow depth with minimum specific energy for a given discharge. At this depth the Froude number is 1, which marks the transition between deep, slower subcritical flow and shallow, faster supercritical flow.
General critical-flow condition
Q2T / (gA3) = 1
Rectangular channel formula
yc = [Q2 / (gb2)]1/3
Enter discharge as cfs with dimensions in feet, or m3/s with dimensions in metres. The calculator reports yc, critical velocity in ft/s or m/s, and minimum specific energy.
Critical depth is the depth at which specific energy is minimum for a given discharge. At critical depth, the Froude number equals 1 and flow transitions between subcritical and supercritical regimes.
Key relationships:
For rectangular channels: yc = (Q2 / (g * b2))1/3
For educational purposes only. Not a substitute for professional engineering judgment.
Interactive model
Rotate the channel model and compare flow depth with the critical-depth section where specific energy is minimized.
Open full model (opens in a new tab)Critical depth occurs where the specific energy of the flow is at a minimum for a fixed discharge. Setting the derivative of specific energy with respect to depth to zero gives the general critical-flow condition, expressed as a section factor:
Z = A3/2 / T1/2 = Q / √g
where, at the critical section:
Equivalently, the flow is critical when the Froude number equals 1, where Dh = A / T is the hydraulic depth:
Fr = V / √(g · Dh) = 1
For simple geometries the equation has a direct (closed-form) solution. For circular pipes and trapezoidal channels there is no closed form, so the calculator solves Z(y) = Q/√g iteratively with a Newton-Raphson method and a bisection fallback, converging to a tolerance of 1×10-8.
Closed-form solutions used for the simple shapes:
Method and equations after Chow, Open-Channel Hydraulics (1959), Chapter 4, and FHWA HEC-22.
The critical-flow condition A3/2/T1/2 = Q/√g applies to every section. The table summarises the geometry and the resulting solution method.
| Shape | Area A | Top width T | Critical depth solution |
|---|---|---|---|
| Rectangular | b·y | b | yc = (Q²/(g·b²))1/3 (direct) |
| Triangular | z·y² | 2·z·y | yc = (2Q²/(g·z²))1/5 (direct) |
| Trapezoidal | (b + z·y)·y | b + 2·z·y | Iterative (Newton-Raphson) |
| Circular | Partial-flow area (θ) | Chord width (θ) | Iterative (Newton-Raphson) |
b = bottom width, y = depth, z = side slope (horizontal:vertical), θ = subtended angle of the wetted circular segment. For a rectangular channel Dh = y; for a triangular channel Dh = y/2.
The same critical-flow condition applies to every section, but the geometry changes A and T. These examples can be reproduced with the calculator above.
For Q = 100 cfs and b = 10 ft, the direct formula gives yc = 1.46 ft, Vc = 6.85 ft/s, and Emin = 2.19 ft.
For Q = 50 cfs and symmetric z = 2H:1V side slopes, yc = [2Q2/(gz2)]1/5 = 2.08 ft.
For Q = 50 cfs, b = 8 ft, and z = 2H:1V, the numerical solution of Q2T/(gA3) = 1 gives yc = 0.979 ft.
For Q = 10 cfs in a 4 ft diameter pipe, solving with circular-segment area and top width gives yc = 0.921 ft (yc/D = 0.230).
Rectangular and triangular values are verification cases based on Chow (1959); trapezoidal and circular values use the same iterative geometry solver as the calculator.
Critical depth acts as a control section — at culvert inlets/outlets, weirs, flumes and free overfalls — that sets a known depth-discharge relationship for backwater and water-surface-profile calculations.
Comparing normal depth to critical depth tells you whether flow is subcritical or supercritical, locates hydraulic jumps, and informs energy-dissipation and stilling-basin design. Avoid designing in the unstable near-critical band (Fr 0.9–1.1).
Critical depth (y_c) is the flow depth at which the specific energy is minimum for a given discharge. At this depth the Froude number equals 1, and the flow is right at the transition between subcritical (tranquil, deep, slow) and supercritical (rapid, shallow, fast) flow. It depends only on the discharge and the channel geometry — not on the channel slope or roughness.
Critical depth is found by solving the section-factor equation A^(3/2) / T^(1/2) = Q / sqrt(g), where A is flow area, T is top width, Q is discharge and g is gravitational acceleration. For rectangular and triangular channels this has a closed-form solution; for circular pipes and trapezoidal channels it must be solved iteratively. This calculator uses a Newton-Raphson solver with a bisection fallback to converge on y_c.
Compare the actual (normal) flow depth to the critical depth. If the flow depth is greater than y_c, the Froude number is below 1 and the flow is subcritical. If the flow depth is less than y_c, the Froude number is above 1 and the flow is supercritical. At y_c exactly, Fr = 1. Near-critical flow (roughly Fr between 0.9 and 1.1) is unstable and should be avoided in design.
By definition, critical depth is the depth where the Froude number equals 1, so the calculator reports Fr ~ 1.0 as a verification check that it converged on the true critical section. A value of 1.000 confirms the geometry, discharge and solver are all consistent. Small deviations indicate an iterative solution that has not fully converged.
Calculates the critical depth in an open channel or pipe — the depth at which specific energy is minimized and the Froude number equals 1.
Critical depth depends only on discharge and channel geometry, not on roughness or slope. Ensure the cross-section dimensions accurately represent the channel at the location of interest.
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Last verified: February 2026