Summarizing Viscosity and Laminar Flow
Summary
- Laminar flow is characterized by smooth flow of the fluid in layers that do not mix.
- Turbulence is characterized by eddies and swirls that mix layers of fluid together.
- Fluid viscosity \(\eta \) is due to friction within a fluid. Representative values are given in this table. Viscosity has units of \(({\text{N/m}}^{2})\text{s}\) or \(\text{Pa}\cdot \text{s}\).
- Flow is proportional to pressure difference and inversely proportional to resistance:
\(Q=\cfrac{{P}_{2}-{P}_{1}}{R}.\)
- For laminar flow in a tube, Poiseuille’s law for resistance states that
\(R=\cfrac{8\eta l}{{\mathrm{\pi r}}^{4}}.\)
- Poiseuille’s law for flow in a tube is
\(Q=\cfrac{({P}_{2}-{P}_{1})\pi {r}^{4}}{8\eta l}.\)
- The pressure drop caused by flow and resistance is given by
\({P}_{2}-{P}_{1}=RQ.\)
Glossary
laminar
a type of fluid flow in which layers do not mix
turbulence
fluid flow in which layers mix together via eddies and swirls
viscosity
the friction in a fluid, defined in terms of the friction between layers
Poiseuille’s law for resistance
the resistance to laminar flow of an incompressible fluid in a tube: R = 8ηl/πr4
Poiseuille’s law
the rate of laminar flow of an incompressible fluid in a tube: Q = (P2 − P1)πr4/8ηl
This lesson is part of:
Fluid Dynamics and Applications
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