mech
Fluid Dynamics: Bernoulli, Boundary Layer & Pipe Losses
From Bernoulli's equation to Darcy-Weisbach and Navier-Stokes — the head-loss calculation interviewers make you do on the spot.
ThermaxISROTata MotorsBoschL&T Heavy Engineering
Key formulas
p1/ρg + v1²/2g + z1 = p2/ρg + v2²/2g + z2 + h_loss
Bernoulli equation: Head form; add losses to model real flow between two sections.
hf = f·(L/d)·(v²/2g)
Darcy-Weisbach: Major loss in pipes; f from Reynolds number and relative roughness (Moody chart).
Re = ρvd/μ = vd/ν
Reynolds number: Ratio of inertial to viscous forces — the flow-regime decider for every internal flow.
Cheat sheet
- ▸Bernoulli: p + ½ρv² + ρgz = constant along a streamline for steady, incompressible, inviscid, non-rotating flow — every term is a form of energy per unit volume.
- ▸Reynolds number Re = ρvd/μ decides laminar (Re < 2300, pipes) vs turbulent; laminar friction factor f = 64/Re, turbulent from the Moody chart / Colebrook equation.
- ▸Darcy-Weisbach: hf = f·(L/d)·(v²/2g) — the universal head-loss equation; minor losses use K·v²/2g (entrance 0.5, sudden expansion (v1−v2)²/2g, exit 1).
- ▸Boundary layer: thickness grows with x^½; separation occurs where the wall shear becomes zero under an adverse pressure gradient (dp/dx > 0) — the cause of bluff-body wakes.
- ▸Navier-Stokes = Newton's second law per unit volume for a viscous fluid; dropping viscosity gives Euler equations, dropping everything gives Bernoulli.
- ▸Continuity: A1v1 = A2v2 for incompressible flow — the first equation to write in any pipe-network problem.
Laminar vs turbulent pipe flow
| Aspect | Laminar | Turbulent |
|---|---|---|
| Re (pipes) | < 2300 | > 4000 |
| Friction factor | 64/Re (independent of roughness) | Moody / Colebrook (roughness matters) |
| Velocity profile | Parabolic, v_max = 2·v_avg | Flatter, logarithmic, v_max ≈ 1.2·v_avg |
| Mixing | Diffusion only | Rapid mixing, better heat transfer |
| Analysis | Exact (Hagen-Poiseuille) | Empirical correlations |
Visual
Venturi / Bernoulli application: A1 large A2 throat ┌──────\ /──────┐ │ p1, v1 → p2, v2 → │ p2 < p1, v2 > v1 (A2 < A1) └──────/ \──────┘ Pitot tube: stagnation point → v = √(2·(p0 − p)/ρ)
Top 4 campus interview questions
MCQ mastery quiz
1. Bernoulli's equation is valid for…
2. Laminar flow in a pipe occurs below Reynolds number…
3. For laminar pipe flow, the friction factor equals…
4. Head loss in a pipe by Darcy-Weisbach is proportional to…