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Definitions of basic fluid properties

Short answer

Specific weight is weight per unit volume (γ = ρg). Specific gravity is density ratio to water. Specific mass is mass per unit volume. Specific volume is volume per unit mass. Viscosity resists shear (τ = μ du/dy). Surface tension is force per length on a surface. Capillarity is liquid rise/fall in a tube (h = 4σ cosθ/(ρ g d)). Compressibility is fractional volume change per pressure change.

Define the terms specific weight, specific gravity, specific mass, specific volume, viscosity, surface tension, capillarity and compressibility.

These are the basic physical properties used to describe a fluid.

  • Specific weight (weight density), ww or γ\gamma: weight per unit volume, γ=ρg\gamma = \rho g. Unit N/m³. Water: 9810 N/m³.
  • Specific gravity, SS: ratio of the density (or specific weight) of a fluid to that of a standard fluid (water at 4 °C for liquids, air for gases). S=ρ/ρwS = \rho/\rho_w; no unit. Mercury: 13.6.
  • Specific mass (mass density), ρ\rho: mass per unit volume, ρ=m/V\rho = m/V. Unit kg/m³. Water: 1000 kg/m³.
  • Specific volume, vv: volume per unit mass, v=1/ρv = 1/\rho. Unit m³/kg. Mostly used for gases.
  • Viscosity: the property by which a fluid resists the relative motion (shear) between its layers. By Newton's law, τ=μdudy\tau = \mu \dfrac{du}{dy}, where μ\mu is the dynamic viscosity (N·s/m² or Pa·s). Kinematic viscosity ν=μ/ρ\nu = \mu/\rho (m²/s).
  • Surface tension, σ\sigma: the tensile force per unit length acting on the free surface of a liquid, caused by cohesion between liquid molecules. Unit N/m. Water–air at 20 °C: about 0.073 N/m.
  • Capillarity: rise or fall of a liquid in a thin tube due to surface tension, adhesion and cohesion. Rise h=4σcos⁡θρgdh = \dfrac{4\sigma \cos\theta}{\rho g d}. Water rises (adhesion > cohesion); mercury falls.
  • Compressibility: the reciprocal of bulk modulus; it measures the fractional change in volume per unit change of pressure, β=1K=−dV/Vdp\beta = \dfrac{1}{K} = -\dfrac{dV/V}{dp}. Unit m²/N. Liquids have very low compressibility, so they are treated as incompressible.

✓ Answer checked by Claude Opus 5.5 (high effort)

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