FLUID MECHANICS · 01–02 / BASIC
Density, pressure & viscosity
Definitions, SI units, validity conditions and a worked water-property example for density, pressure and viscosity in fluid mechanics.
Abstract
Density measures mass per unit volume, pressure is the isotropic normal stress in a fluid at rest, and viscosity quantifies resistance to the rate of deformation. Together they characterize inertia, mechanical state and momentum transport.
Density: connecting mass and volume
For a uniform sample, mean density ρ is mass m divided by volume V. Continuum mechanics uses a local field ρ(x, t), defined over a sampling volume that is small macroscopically but still large relative to molecular scales.
Liquid density is often treated as constant over ordinary pressure ranges. Gas flows, high-speed flows and problems with large temperature differences generally require density to vary with pressure and temperature.
- Density[]
- Mass[]
- Volume[]
- Physical role
- Appears in mass conservation and inertia; it fixes how much matter occupies a given volume.
- State dependence
- Generally depends on temperature and pressure and may change abruptly across a phase boundary.
Pressure: stress normal to a surface
In a fluid at rest, the stress acting across any plane through a point is normal to that plane and independent of its orientation. Its magnitude is pressure p. When the stress is nearly uniform over a finite area, it can be evaluated as normal force Fₙ divided by area A. The pascal is defined by 1 Pa = 1 N/m² [1].
Absolute pressure uses perfect vacuum as its zero; gauge pressure uses the surrounding atmospheric pressure. Equations of state and comparisons with vapor pressure normally require absolute pressure.
- Pressure[]
- Normal force[]
- Loaded area[]
- Absolute pressure[]
- Gauge pressure[]
- Ambient atmospheric pressure[]
Viscosity: transport of momentum across velocity gradients
Consider simple shear, u = u(y). In a Newtonian fluid, shear stress τ is proportional to shear rate du/dy; the coefficient μ is the dynamic viscosity, not the kinematic viscosity [2, 3].
Kinematic viscosity ν is μ divided by density ρ and is useful when comparing viscous momentum diffusion with inertia. Both μ and ν depend on temperature; for liquids, μ generally decreases as temperature rises.
- Shear stress[]
- Dynamic viscosity[]
- Shear rate[]
- Kinematic viscosity[]
- Dynamic viscosity[]
- Density[]
- Newtonian fluid
- Stress and shear rate are linearly related, so μ can be treated as a state-dependent material property.
- Non-Newtonian fluid
- Paints, slurries and polymer solutions may have an apparent viscosity that depends on shear rate or flow history.
Worked example: kinematic viscosity of water at 20 °C
For water near 0.1 MPa and 20 °C, use the representative rounded values ρ = 998.2 kg/m³ and μ = 1.002 × 10⁻³ Pa·s. These values are consistent with the IAPWS-based reference correlations described by NIST; precision work should evaluate the standard formulations at a stated temperature and pressure [4, 5].
Substitution in Equation (5) gives ν = (1.002 × 10⁻³) / 998.2 ≈ 1.004 × 10⁻⁶ m²/s. A property-table value should always be reported with temperature, pressure, units and appropriate significant figures.
| Quantity | Symbol | Value | SI unit |
|---|---|---|---|
| Density | ρ | 998.2 | kg/m³ |
| Dynamic viscosity | μ | 1.002 × 10⁻³ | Pa·s |
| Kinematic viscosity | ν | 1.004 × 10⁻⁶ | m²/s |
References
Sources accessed 13 August 2026. Independent expert review has not yet been completed.
- [1] BIPM, The International System of Units (SI Brochure), 9th ed., ver. 4.01, 2026.↗
- [2] IUPAC Gold Book, “Newtonian fluid,” 5th ed.↗
- [3] IUPAC Gold Book, “shear viscosity,” 5th ed.↗
- [4] NIST, Contributions to International Standards on the Properties of Water.↗
- [5] NIST, Reference Correlations for Thermophysical Properties of Liquid Water at 0.1 MPa.↗