1.5324
m/s
3.0648
m³/s
38.4615
m
0.002
m²
1.5324
m/s
3.0648
m³/s
38.4615
m
0.002
m²
The Manning's Equation Calculator computes the mean velocity and discharge in an open channel using Manning's formula, the most widely used equation in open-channel hydraulics. Developed empirically by Robert Manning in 1889, it relates flow velocity to channel geometry and roughness: $$v = \frac{1}{n} R_h^{2/3} S^{1/2}$$ where n is Manning's roughness coefficient, R_h is the hydraulic radius, and S is the energy slope (approximated by the bed slope for uniform flow).
The discharge follows from continuity: $$Q = v \cdot A = \frac{A}{n} R_h^{2/3} S^{1/2}$$
Manning's equation is the workhorse of civil and environmental engineering — used to design drainage channels, size culverts, analyze flood plains, design irrigation systems, and evaluate river capacity. The roughness coefficient n captures the combined effect of bed material, vegetation, channel irregularity, and obstructions. Published tables provide n values for hundreds of channel types, from smooth concrete (n ≈ 0.012) to heavily vegetated floodplains (n ≈ 0.15).
Manning's equation is an empirical formula for uniform, steady, open-channel flow. It assumes the flow is fully developed and the depth, velocity, and cross-section remain constant along the channel (normal flow).
Velocity: $$v = \frac{1}{n} R_h^{2/3} S^{1/2}$$
Hydraulic radius: $$R_h = \frac{A}{P}$$ where A is the cross-sectional flow area and P is the wetted perimeter. For a wide, shallow channel, R_h ≈ depth.
Common n values: Smooth concrete: 0.012 | Clean earth: 0.022 | Gravel: 0.025 | Natural stream (clean): 0.030 | Natural stream (weeds): 0.050 | Floodplain (heavy brush): 0.10–0.15
The slope S is the energy grade line slope, which equals the bed slope for uniform flow (normal depth). For gradually varied flow, the actual energy slope differs from the bed slope.
A smaller n value (smoother channel) yields higher velocity for the same geometry and slope. Velocity increases with hydraulic radius (larger or more efficient cross-section) and with steeper slope. The 2/3 exponent on R_h means that velocity is less sensitive to changes in depth than to changes in roughness. The discharge Q = vA combines velocity and area effects — doubling the area more than doubles discharge because the larger area also increases R_h.
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Results
A smooth concrete channel (n = 0.013) with Rh = 0.5 m and 0.2% slope produces v ≈ 2.17 m/s. With 2 m² cross-section, Q ≈ 4.33 m³/s.
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Results
A natural stream (n = 0.030) with Rh = 0.8 m and gentle 0.05% slope flows at ~0.64 m/s. Despite the larger area, the rougher channel and gentler slope reduce velocity compared to the concrete channel.
Manning's n is an empirical coefficient representing the frictional resistance of the channel boundary. It depends on surface roughness, vegetation, channel irregularity, and obstructions. Values range from about 0.010 for glass/smooth PVC to over 0.15 for dense floodplain vegetation. Published tables (e.g., Chow 1959) provide values for hundreds of channel types.
Yes, Manning's equation works for partially filled pipes (open-channel flow) and is commonly used in sewer design. For full-pipe (pressurized) flow, the Darcy-Weisbach or Hazen-Williams equations are more appropriate.
They are mathematically related. Chezy's formula is v = C√(Rh·S). Manning's equation can be seen as a specific form of Chezy's where C = (1/n)·Rh^(1/6). Manning's is more popular because n varies less with depth than C does.
In US customary units (feet, seconds), the formula includes a conversion factor: v = (1.486/n)·Rh^(2/3)·S^(1/2). This calculator uses SI units (meters). Multiply the velocity by 1.486 and use feet for US customary results.
Uniform flow means the depth, velocity, and cross-section are constant along the channel. This occurs when the gravitational driving force exactly balances frictional resistance, creating a flow at 'normal depth.' Manning's equation strictly applies to this condition.
The most hydraulically efficient shape maximizes the hydraulic radius Rh = A/P. For open channels, the semicircle is optimal. Among practical shapes, a trapezoid with 60° sides is most efficient. A wider, shallower channel is less efficient than a narrower, deeper one with the same area.
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