Continuity
Mass is conserved in a flow. Learn mass and volume flow rate, the continuity equation A₁V₁ = A₂V₂, flow in branching pipes, and compressible mass flow.
Put your thumb over a garden hose and the water shoots out faster. Nothing is created or lost — the same amount of water per second must pass through a smaller opening, so it speeds up. That's the continuity equation.
It is the first equation written for every pipe network, duct, nozzle and pump system.
An analogy
Traffic on a motorway narrowing from three lanes to one: if the same number of cars per minute must pass, they have to go faster in the narrow section.
Flow rate
Volume flow rate is area × average velocity. 1 m³/s = 1000 L/s = 3600 m³/h. A domestic tap delivers about 0.1–0.2 L/s.
Velocity and diameter
For round pipes, V ∝ 1/D². Halving the diameter quadruples the velocity. Designers choose pipe size to keep water velocity ≈ 1–3 m/s (noise, erosion, pressure loss vs pipe cost).
Networks
At every junction, flow in = flow out (like Kirchhoff's current law). Combined with energy losses around loops, this solves water-distribution networks (Hardy Cross method).
Differential form and compressible flow
The differential form ∂ρ/∂t + ∇·(ρV) = 0 is one of the Navier–Stokes equations solved by CFD. In compressible nozzle flow, mass flow per area peaks at Mach 1 (choked flow) — limiting flow through valves and orifices.
Formulas
- Flow rate:
Q = A · V, ṁ = ρ A V - Incompressible continuity:
A₁V₁ = A₂V₂ - Compressible:
ρ₁A₁V₁ = ρ₂A₂V₂ - Junctions:
ΣQ_in = ΣQ_out
Worked example: Pipe reducer
Given: 100 mm pipe at 2 m/s; Reduces to 50 mm
Find: Flow rate and velocity in the small pipe.
- Q = π/4 × 0.1² × 2 = 0.0157 m³/s = 15.7 L/s
- V₂ = 2 × (100/50)² = 8 m/s
Answer: 15.7 L/s, 8 m/s
Worked example: Branch
Given: Main carries 20 L/s; Branch A takes 12 L/s through 80 mm pipe
Find: Flow and velocity in branch A, flow in branch B.
- V_A = 0.012/(π/4 × 0.08²) = 2.39 m/s
- Q_B = 20 − 12 = 8 L/s
Answer: 2.39 m/s; 8 L/s in B
Common mistakes
- Wrong: Using diameter instead of area ratio. — Right: V₂/V₁ = (D₁/D₂)², not D₁/D₂.
- Wrong: Using A₁V₁ = A₂V₂ for high-speed gas flow. — Right: Include density: ρ₁A₁V₁ = ρ₂A₂V₂.
Applications
- Water supply: Main and branch sizing for buildings and cities.
- Nozzles & jets: Fire hoses, pressure washers and fuel injectors speed fluid up by reducing area.
- HVAC ducts: Duct sizing keeps air velocity low enough to avoid noise.
Key takeaways
- Q = AV; ṁ = ρAV.
- A₁V₁ = A₂V₂ for liquids.
- V ∝ 1/D² — size pipes for 1–3 m/s water.
- Junctions: flow in = flow out.
Going further
- Choked flow: Gas flow through a restriction maxes out when the throat reaches sonic speed — used in critical-flow nozzles for calibration.
- Unsteady continuity: Tank filling: A dh/dt = Q_in − Q_out.
- CFD: Finite-volume solvers enforce continuity in every cell; pressure-correction algorithms (SIMPLE) exist to satisfy it.