Dynamic viscosity (also known as absolute viscosity) is the measurement of the fluid's internal resistance to flow.
The sources are:
Sutherland's formula can be used to derive the dynamic viscosity of an ideal gas as a function of the temperature. According to Sutherland's formula, if the absolute temperature is less than $S_{gas}$, the relative change in viscosity for a small change in temperature is greater than the relative change in the absolute temperature, but it is smaller when $T_{gas}$ is above $S_{gas}$. The kinematic viscosity though always increases faster than the temperature.
Note: Often called $\mu$ instead of $\eta$
Note: 1 Pa = 1 kg/(m.s$^2$)
$1.715747771{\cdot}{10}^{-5}+4.722402075{\cdot}{10}^{-8} \theta_{gas}-3.663027156{\cdot}{10}^{-10} {\theta_{gas}}^2+1.873236686{\cdot}{10}^{-12} {\theta_{gas}}^3-8.050218737{\cdot}{10}^{-14} {\theta_{gas}}^4$ | humid air @ 1 atm (Tsilingiris2007) |
${10}^{-6}\frac{1.4592{T_{gas}}^{\frac{3}{2}}}{109.1+T_{gas}}$ | dry air @ 1 bar (UW/MHTL 8406, 1984) |
${10}^{-6}\left(-9.8601{\cdot}{10}^{-1}+9.080125{\cdot}{10}^{-2} T_{gas}-1.17635575{\cdot}{10}^{-4} {T_{gas}}^2+1.2349703{\cdot}{10}^{-7} {T_{gas}}^3-5.7971299{\cdot}{10}^{-11} {T_{gas}}^4\right)$ | dry air @ at 1 atm (Irvine&Liley1984) |
$1.66{\cdot}{10}^{-5}+4.14{\cdot}{10}^{-8} \theta_{gas}$ | N2 (Vermeer1983) |
$1.47{\cdot}{10}^{-5}+4.11{\cdot}{10}^{-8} \theta_{gas}$ | SF6 (Vermeer1983) |
$1.11{\cdot}{10}^{-6}+4.669{\cdot}{10}^{-8} \left(\theta_{gas}+\theta_{abs}\right)$ | CO2 (linear interpolation) |
$\nu_{gas} \rho_{gas}$ | general formula for gases |
$\eta 0_{gas} \frac{T0_{gas}+S_{gas}}{T_{gas}+S_{gas}} \left(\frac{T_{gas}}{T0_{gas}}\right)^{1.5}$ | Sutherland's model |
Gas | Formula | 0°C | 15°C | 25°C | 50°C | 75°C | 100°C |
---|---|---|---|---|---|---|---|
Air | 78%N2+21%O2+minor | 1.7218e-05 | 1.7962e-05 | 1.8447e-05 | 1.9601e-05 | 2.0721e-05 | 2.018e-05 |
N2 | N2 | 1.6629e-05 | 1.7339e-05 | 1.7805e-05 | 1.8947e-05 | 2.0044e-05 | 2.1108e-05 |
SF6 | SF6 | 1.3771e-05 | 1.4589e-05 | 1.5123e-05 | 1.6675e-05 | 1.7786e-05 | 0.001888 |
CO2 | CO2 | 1.3711e-05 | 1.4446e-05 | 1.4932e-05 | 1.6134e-05 | 1.7315e-05 | 1.8475e-05 |
CO | CO | 1.6515e-05 | 1.7201e-05 | 1.7649e-05 | 1.8741e-05 | 1.9794e-05 | 2.0813e-05 |
O2 | O2 | 1.9143e-05 | 1.9993e-05 | 2.055e-05 | 1.8741e-05 | 1.9794e-05 | 2.0813e-05 |
H2 | H2 | 8.3969e-06 | 8.7098e-06 | 8.9154e-06 | 9.4193e-06 | 9.9103e-06 | 1.0389e-05 |
NH3 | NH3 | 9.1931e-06 | 9.7289e-06 | 1.0093e-05 | 1.102e-05 | 1.1968e-05 | 1.2929e-05 |
SO2 | SO2 | 1.1796e-05 | 1.2475e-05 | 1.2924e-05 | 9.589e-05 | 1.0664e-05 | 1.1739e-05 |
He | He | 1.8695e-05 | 1.9388e-05 | 1.9846e-05 | 2.0971e-05 | 2.2073e-05 | 2.3154e-05 |
Ar | Ar | 2.1017e-05 | 2.1987e-05 | 2.2624e-05 | 2.4114e-05 | 2.5624e-05 | 2.7093e-05 |
Kr | Kr | 2.3219e-05 | 2.4375e-05 | 2.5132e-05 | 2.6984e-05 | 2.8774e-05 | 3.0509e-05 |
Xe | Xe | 2.1216e-05 | 2.2278e-05 | 2.2985e-05 | 2.4745e-05 | 2.6493e-05 | 2.8224e-05 |
Ne | Ne | 2.9382e-05 | 3.0427e-05 | 3.1113e-05 | 3.2791e-05 | 3.4419e-05 | 3.6005e-05 |