Weir Flow Calculator
Calculate discharge over a rectangular or 90° V-notch sharp-crested weir from crest length and head using the Francis and Kindsvater-Shen equations (Cd =
Weir Flow Calculator
Calculator
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Formula: Rectangular: Q = (2/3)Cd × L × √(2g) × H^(3/2) | Triangular (90°): Q = (8/15)Cd × √(2g) × tan(θ/2) × H^(5/2)
Worked example — Q ≈ 0.60 m³/s (602 L/s)
Formula
Rectangular: Q = (2/3)Cd × L × √(2g) × H^(3/2) | Triangular (90°): Q = (8/15)Cd × √(2g) × tan(θ/2) × H^(5/2)
Francis formula for rectangular weirs (Cd≈0.62). Kindsvater-Shen for triangular (V-notch) weirs. g = 9.81 m/s².
Worked Examples
Example 1: Rectangular sharp-crested weir
Problem:Crest length L = 2 m, head H = 0.3 m, Cd = 0.62
Solution:Q = (2/3) × 0.62 × 2 × √(2 × 9.81) × 0.3^1.5 = 0.8267 × 4.429 × 0.1643 = 0.602 m³/s
Result:Q ≈ 0.60 m³/s (602 L/s)
Example 2: 90° V-notch weir at low flow
Problem:Head H = 0.15 m, θ = 90°, Cd = 0.62
Solution:Q = (8/15) × 0.62 × √(2 × 9.81) × tan(45°) × 0.15^2.5 = 0.3307 × 4.429 × 1 × 0.008714 = 0.01276 m³/s
Result:Q ≈ 0.0128 m³/s (12.8 L/s)
Example 3: Doubling the head on a rectangular weir
Problem:Same 2 m weir, head raised from 0.3 m to 0.6 m
Solution:Q scales with H^1.5, so Q2/Q1 = (0.6/0.3)^1.5 = 2.83 Q2 = 0.602 × 2.83 = 1.70 m³/s
Result:Q ≈ 1.70 m³/s — doubling the head almost triples the discharge
Frequently Asked Questions
When to use V-notch vs rectangular weir?
V-notch (triangular) weirs are more accurate at low flows. Rectangular weirs handle higher flows and are simpler to construct.
What is the discharge coefficient Cd and how is it determined?
The discharge coefficient (Cd) accounts for real-world flow effects not captured in the theoretical formula, including boundary layer effects, velocity of approach, and surface tension. For sharp-crested rectangular weirs, Cd is typically 0.62-0.64. V-notch weirs typically have Cd around 0.58-0.62. Cd values are determined through laboratory calibration using measured flow rates and can vary with head, weir geometry, and channel approach conditions.
What precautions are needed for accurate weir flow measurement?
For accurate measurements, the approach channel should be straight and at least 10-20 times the maximum head length upstream to allow uniform flow. The weir crest should be level and sharp-edged, and the nappe (water sheet) must spring clear of the weir plate. The head should be measured at least 3-4 times the maximum head distance upstream to avoid the drawdown zone near the weir. Submerged tailwater conditions invalidate standard weir formulas and require correction factors.
What head values are practical for V-notch and rectangular weirs?
V-notch weirs (90° notch) are accurate for heads between about 0.06 m and 0.38 m, making them suitable for small stream monitoring, irrigation channels, and laboratory flow measurement. Rectangular weirs are practical for heads from 0.05 m to 0.60 m with crest lengths up to several meters, suitable for irrigation canals, drainage channels, and wastewater treatment plants. Very low heads increase measurement error due to surface tension and approach velocity effects.
Why is discharge proportional to head to the 3/2 power for a rectangular weir but 5/2 for a V-notch?
The velocity of a free jet at depth h below the surface follows Torricelli, varying with the square root of h. For a rectangular notch the flow width is constant, so integrating the square root of h over the depth of the overfall gives head to the 3/2 power. In a triangular notch the width itself grows in proportion to depth, adding one more power of head to the integrand and producing the 5/2 exponent. That steeper exponent is what gives the V-notch its sensitivity at low flow.
What is an end contraction, and how does the Francis correction handle it?
When a rectangular notch is narrower than the approach channel, the streamlines curve inward at each side and the effective width of the nappe is less than the physical crest length. Francis, from his full-scale tests at Lowell, proposed reducing the crest length by 0.1 times the head for each contraction, giving an effective length of L minus 0.1 x n x H, with n equal to 2 for a fully contracted notch and 0 for a suppressed weir spanning the whole channel. Ignoring it overstates discharge.
What happens when the tailwater rises above the weir crest?
The weir becomes submerged or drowned, and the free-discharge equations no longer apply, because downstream depth now influences the flow as well as upstream head. Discharge for a given upstream head falls, so a standard weir reading will overstate the true flow, sometimes badly. Submerged operation is handled with an empirical reduction factor based on the ratio of downstream to upstream head, but accuracy degrades sharply. Good practice is to set the crest high enough that tailwater never reaches it.
Why does the nappe have to be ventilated?
A sharp-crested weir assumes the underside of the falling sheet is at atmospheric pressure. If the space beneath the nappe is sealed, the falling water entrains air out of that pocket and the pressure drops, drawing the sheet toward the plate. A depressed or clinging nappe passes more flow at the same head than the equation predicts, so readings under-report discharge and the sheet may oscillate noisily. Vent pipes or side openings that admit air to the cavity restore the assumed condition.
How does an error in the head reading propagate into the calculated flow?
Because discharge is a power of head, relative errors are amplified by the exponent. For a rectangular weir a 1 percent error in H produces about 1.5 percent error in Q; for a 90 degree V-notch the amplification is 2.5 times. This is why head is measured with a hook gauge or a stilling well rather than a tape held in flowing water, and why very small heads are avoided: the same few millimetres of reading error becomes a much larger percentage of a shallow head.
How does a sharp-crested weir differ from a broad-crested weir or a flume?
A sharp-crested weir uses a thin plate so the nappe springs clear, and its coefficient reflects that free overfall. A broad-crested weir has a crest long enough in the flow direction for the water to pass through critical depth on top of it, which gives a different rating relation and tolerates submergence better. A Parshall or long-throated flume forces critical flow by contracting the channel instead, causing little head loss and passing sediment, which suits wastewater and irrigation channels where a weir pool would silt up.
References
Background & Theory
History
Reviewed for accuracy by Daniel Agrici, Founder & Lead Developer · Editorial policy
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