Conserve mass flow without inventing a branch split
In timeΔt, fluid moving at mean speedv through cross-sectional areaA transports volumeAvΔt. Its volume flow rate isQ=Av and mass flow rate isρAv. A steady control volume has no accumulating mass, so incoming mass flow equals total outgoing mass flow. For the same incompressible fluid, density cancels and the volume flows balance.
Learning outcome: At inlet speed1, compare branch fractions0.25,0.5 and0.75. Reconstruct eachQ from its own area and speed, then sum. Change inlet speed while fixing the split and predict all flow ratios before capture. State why the fraction requires independent information.
Starting recap
Review density and unit conversion, perpendicular force components, static force balance, work-energy, mass conservation and projectile motion.
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Try
An inlet area0.004 m² and speed1 m/s carryQ=0.004 m³/s. If half enters each branch, areas0.001 and0.002 m² produce speeds2 and1 m/s. Each branch carries0.002 m³/s; total mass flow forρ1000 is4 kg/s. Unequal speeds do not imply unequal branch volume flows.
Open the experimentPredict
Can two branches have equal flow rates but different speeds?
Experiment
At inlet speed1, compare branch fractions0.25,0.5 and0.75. Reconstruct eachQ from its own area and speed, then sum. Change inlet speed while fixing the split and predict all flow ratios before capture. State why the fraction requires independent information.
Close a branching incompressible volume balance
Worked teaching model · synthetic values · Steady fully filled incompressible flowρ1000 kg/m³. Inlet area0.004 m²; branch areas0.001 and0.002 m². Branch fraction is supplied, not inferred from area or pressure. No accumulation or leakage.
Reset keeps your prediction, captures and practice history.
| Quantity | Value | Unit |
|---|---|---|
| Inlet volume flow | 0.004 | m³/s |
| Branch-one volume flow | 0.002 | m³/s |
| Branch-two volume flow | 0.002 | m³/s |
| Branch-one mean speed | 2 | m/s |
| Branch-two mean speed | 1 | m/s |
| Total mass flow | 4 | kg/s |
Accessible plot coordinates
| coordinate | value |
|---|
Incoming volume flow equals the sum of outgoing flows in a steady incompressible junction.
Q=Av and mass flow=ρQ. Continuity alone cannot determine an unknown branch split: pressure and flow resistance or other boundary information are needed. Area varies as radius squared. A fluid element can accelerate by changing direction even if its speed is unchanged.
Incoming volume flow equals the sum of outgoing flows in a steady incompressible junction.
Q=Av and mass flow=ρQ. Continuity alone cannot determine an unknown branch split: pressure and flow resistance or other boundary information are needed. Area varies as radius squared. A fluid element can accelerate by changing direction even if its speed is unchanged.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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How can a fluid particle accelerate inside a steady pipe flow?
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