Laboratory Tilting Hydraulics Flume
Glass-walled rectangular flume (0.30 m width, 8.0 m length) with variable slope control.
Investigate hydraulic jump formation, measure initial and sequent flow depths, compute head loss and energy dissipation efficiency, and verify the classical Bélanger momentum equation in a tilting flume. Explore interactive structural mechanics, materials simulation, and civil engineering telemetry.
Ready to sample with Predictor F(Fr_1) = 2.5 ratio.
Adjust Predictor F(Fr_1), then execute civil engineering measurement.
Civil engineering telemetry is evaluated rigorously using 64-bit IEEE 754 precision. Residuals reflect ordinary least-squares regression across successive observations. Continuous data structures support high-fidelity structural mechanics and geotechnical continuum modeling.
The civil engineering physical models apply within the specified calibrated operational window (1.5 to 4.5 ratio). Evaluated in an 8-meter tilting flume with adjustable sluice gate and tailwater weir. Linearized relationship correlates measured depth ratio directly to the Bélanger predictor with slope 1.0000.
Glass-walled rectangular flume (0.30 m width, 8.0 m length) with variable slope control.
Sharp-edged vertical gate generating high-velocity supercritical flow sheets.
Controls backwater depth to position and stabilize the hydraulic jump in the flume observation zone.
Simultaneously measures initial depth y_1 and sequent depth y_2 to ±0.05 mm precision.
Traverses flow depth to record upstream and downstream velocity head profiles.
Measures total volumetric discharge Q to ±0.5% reading accuracy.
Investigate hydraulic jump formation, measure initial and sequent flow depths, compute head loss and energy dissipation efficiency, and verify the classical Bélanger momentum equation in a tilting flume. Standardized parameter settings: 1.5, 2.0, 2.5, 3.0, 3.5, 4.0 ratio.
Set flume horizontal; zero hook gauges at flume floor datum; open sluice gate to initial test aperture (e.g. 20 mm).
Start recirculation pump; adjust discharge Q to establish high-velocity supercritical flow beneath the sluice gate.
Raise downstream tailwater weir until a stable, stationary hydraulic jump forms in the middle glass inspection section of the flume.
Position upstream hook gauge immediately upstream of jump roller; record supercritical flow depth y_1; log upstream velocity v_1 = Q / (B · y_1); compute Fr_1.
Position downstream hook gauge immediately downstream of the surface roller where water surface becomes smooth and subcritical; record sequent depth y_2.
Adjust gate aperture and pump discharge across six systematic Froude conditions (predictor = 1.5 to 4.5); record y_1, y_2; calculate energy loss ΔE.
Points are your recorded observations. The solid regression line validates Hydraulic Jump Energy mathematical scaling.
| # | Bélanger Theoretical Predictor F(Fr_1) (ratio) | Measured Sequent Depth Ratio y_2/y_1 (ratio) | Bélanger predictor 0.5·(√(1+8Fr₁²) - 1) | Measured sequent depth ratio y₂/y₁ | Remove |
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No readings yet. Execute a civil engineering trial and record it.
A hydraulic jump is a rapid, highly turbulent open-channel flow phenomenon occurring when supercritical flow (Froude number Fr > 1) abruptly transitions to subcritical flow (Fr < 1). In hydraulic infrastructure—including spillway stilling basins, sluice gate chutes, and canal drop structures—hydraulic jumps are intentionally generated as primary energy dissipators to convert catastrophic kinetic energy into internal thermal turbulence, preventing severe downstream bed scour and riverbank erosion. Applying the one-dimensional momentum conservation equation across the control volume while neglecting boundary friction yields the classical Bélanger equation (1828) relating initial supercritical depth y_1 to subcritical sequent (conjugate) depth y_2: y_2 / y_1 = 0.5 · [√(1 + 8·Fr_1²) - 1], where upstream Froude number Fr_1 = v_1 / √(g·y_1). Specific energy drops dramatically across the jump: head loss ΔE = E_1 - E_2 = (y_2 - y_1)³ / (4·y_1·y_2), representing macro-turbulent roller energy dissipation. Depending on initial Froude number Fr_1, jumps are categorized as undular (1.0 < Fr_1 < 1.7), weak (1.7 < Fr_1 < 2.5), oscillating (2.5 < Fr_1 < 4.5), steady (4.5 < Fr_1 < 9.0), or strong/choppy (Fr_1 > 9.0). In this laboratory flume experiment, supercritical flow is discharged beneath an adjustable sluice gate, and a downstream tailwater weir forces hydraulic jump stabilization to verify conjugate depths and energy dissipation efficiency.
Evaluated in an 8-meter tilting flume with adjustable sluice gate and tailwater weir. Linearized relationship correlates measured depth ratio directly to the Bélanger predictor with slope 1.0000.