Flow
| Specific discharge q | |
| Discharge Q = q·b | |
| V₁ = q/y₁ | |
| Fr₁ = V₁/√(gy₁) | |
| V₂ = q/y₂ | |
| Fr₂ = V₂/√(gy₂) | |
Energy & critical depth
| E₁ = y₁ + q²/(2gy₁²) | |
| E₂ = y₂ + q²/(2gy₂²) | |
| Critical depth y꜀ = (q²/g)^⅓ | |
| E_min = 1.5·y꜀ | |
E = y + q²/(2gy²) · y꜀ = (q²/g)^⅓
Sluice gate rating (lab Eq. 10–11)
| Q_ideal = b·a·√(2gy₁) | |
| C_d = Q/Q_ideal | |
| Energy check E₁ − E₂ | |
Frictionless gate: specific energy is conserved across the gate, so
y₁ (subcritical) and y₂ (supercritical) are alternate depths — the same vertical
line on the E–y diagram. y₂ ≈ a as in the lab manual.
Hump & choking
| Hump height Δz | |
| Choking limit Δz_crit = E₁ − E_min | |
| Depth at crest | |
| Surface drop at crest | |
| Upstream rise (choked) | |
| Energy budget max|E+z−E₁| | |
Over the hump the local specific energy is E(x) = E₁ − z(x):
the operating point slides left along the fixed E–y curve. Once choked, the crest
holds exactly critical flow — the hump has become the control. Downstream the flow
continues supercritical (a jump would follow in a real channel — see the hydraulic-jump
module).