Lesson 41 of 78 · Fluids & Fluid Power
Control Volumes, Pressure & Pipe Flow
A control volume is a boundary through which fluid mass, momentum, and energy can flow. MIT Fluid Dynamics develops pressure, conservation, pipe flow, dimensional analysis, boundary layers, and force from this viewpoint 1.
For steady incompressible flow, \(Q=Av\). Halving flow area doubles mean velocity when the same volumetric flow passes through. The extended energy equation between two points can be organized as
where pump head \(h_p\) adds energy, turbine head \(h_t\) removes it, and \(h_L\) represents losses.
Worked flow-speed check
Water at 18 L/min flows through a 12 mm inside-diameter tube. \(Q=0.0003\) m³/s and \(A=\pi(0.012)^2/4=1.13\times10^{-4}\) m², so mean velocity is 2.65 m/s. If a fitting’s loss coefficient is \(K=1.5\), its pressure-loss estimate is
Add straight-pipe, valve, filter, entrance, and exit losses. Because many losses scale roughly with \(v^2\), an undersized line becomes expensive quickly.
Pressure is not flow
A blocked hydraulic line can have high pressure and zero flow. An open large line can have substantial flow at modest pressure. Pressure creates actuator force \(F=pA\); flow creates ideal actuator speed \(v=Q/A\). The power transferred to an ideal fluid is \(pQ\).
Practice
Map a coolant or hydraulic loop. Mark elevation, diameter, flow, pressure measurement points, valves, filters, and heat sources. Create a loss budget and identify the component most likely to shift with contamination or wear. The circuit should be reviewable without opening a catalog.
Source trail
References
- 1Fluid Dynamics. MIT OpenCourseWare. verifiedUndergraduate course on pressure, control volumes, conservation laws, pipe flow, dimensional analysis, boundary layers, lift, and drag. Cited at: course scope.
Further reading
- University Physics, Volumes 1–3. OpenStax (Rice University). verifiedOpen calculus-based physics. Vol 1 mechanics; Vol 2 thermodynamics and electricity & magnetism; Vol 3 optics & modern physics.
Check your understanding
- For steady incompressible flow in one path, what continuity relation applies?
- Pressure is constant
- Volumetric flow rate is the same through successive sections
- Velocity is always zero
- Pipe diameter cannot change
Conservation of mass gives equal steady volumetric flow through successive sections for an incompressible fluid without branches or leaks.
- Why is Bernoulli’s ideal equation insufficient for a real long pipe?
- It omits viscous and component losses unless extended
- It has too many units
- It forbids pressure
- It only applies to solids
Real systems lose mechanical energy through friction, fittings, valves, and other components.