Overview
Natural gas viscosity at reservoir conditions ranges from 0.01 to 0.06 cp — one to two orders of magnitude lower than oil. Unlike liquids, gas viscosity rises with temperature at low pressure and shows complex P–T behavior at high pressure because density becomes the dominant control. The LGE correlation expresses gas viscosity as an exponential function of gas density, with coefficients that depend on molecular weight and temperature.
Sour-gas reservoirs (H2S, CO2, and N2 content) require two corrections: (1) Wichert-Aziz adjusts the pseudocritical T and P to account for acid-gas effects on Z-factor, and (2) Carr-Kobayashi-Burrows applies an additive viscosity correction proportional to mole fraction of each impurity.
Theory
The full natural-gas viscosity workflow runs four steps: (1) Sutton or Standing correlations give pseudocritical Tpc and Ppc from gas gravity; (2) Wichert-Aziz applies the H2S/CO2 correction if sour; (3) a Z-factor solver (Hall-Yarborough or Dranchuk-Abou-Kassem) gives Z at reduced Tpr/Ppr; and (4) LGE computes viscosity from gas density (derived from Z) and molecular weight.
Formulas
Pseudocritical Properties (Sutton)
Tpc = 169.2 + 349.5*sg - 74.0*sg^2 (deg R)
Ppc = 756.8 - 131.0*sg - 3.6*sg^2 (psia)
sg = specific gravity (air = 1.0). Valid for sweet hydrocarbon gases with sg = 0.55–1.85.
Wichert-Aziz Sour-Gas Correction
A = yH2S + yCO2
B = yH2S
epsilon = 120*(A^0.9 - A^1.6) + 15*(B^0.5 - B^4)
Tpc_corrected = Tpc - epsilon
Ppc_corrected = Ppc * Tpc_corrected / (Tpc + B*(1-B)*epsilon)
yH2S, yCO2 = mole fractions of acid gases. Used in the GPSA Engineering Data Book and SPE textbooks.
Z-Factor (Hall-Yarborough)
t = 1 / Tpr
f(y) = -Ppr_term + (y + y^2 + y^3 - y^4)/(1-y)^3
- (14.76*t - 9.76*t^2 + 4.58*t^3)*y^2
+ (90.7*t - 242.2*t^2 + 42.4*t^3)*y^(2.18 + 2.82*t)
Ppr_term = 0.06125 * Ppr * t * exp(-1.2*(1-t)^2)
Solve f(y) = 0 for y (Newton-Raphson)
Z = Ppr_term / yGas Density
rho_g = (P * M_w) / (Z * R * T)
M_w = 28.96 * sg (molecular weight, lb/lbmol)
R = 10.732 (psia*ft^3 / lbmol / deg R)
P in psia, T in deg R, gives ρg in lb/ft3.
Lee-Gonzalez-Eakin (1966) Viscosity
K = (9.4 + 0.02*M) * T^1.5 / (209 + 19*M + T)
X = 3.5 + 986/T + 0.01*M
Y = 2.4 - 0.2*X
mu_g = 1e-4 * K * exp(X * rho_g^Y)
T in deg R, M = molecular weight in lb/lbmol, ρg in g/cc (or convert), gives μg in cp.
Carr-Kobayashi-Burrows Impurity Corrections
delta_mu_N2 = yN2 * (8.48e-3 * log10(sg) + 9.59e-3)
delta_mu_CO2 = yCO2 * (9.08e-3 * log10(sg) + 6.24e-3)
delta_mu_H2S = yH2S * (8.49e-3 * log10(sg) + 3.73e-3)
mu_g_total = mu_g + delta_mu_N2 + delta_mu_CO2 + delta_mu_H2S
Key Symbols
| Symbol | Description | Units |
|---|---|---|
| mu_g | Gas viscosity | cp |
| rho_g | Gas density at P, T | g/cc |
| Z | Compressibility factor | dimensionless |
| Tpr, Ppr | Pseudoreduced T, P | dimensionless |
| M | Molecular weight | lb/lbmol |
| sg | Gas gravity (air = 1) | dimensionless |
Worked Example
Given: Sweet gas, sg = 0.65, T = 250 °F (710 deg R), P = 4000 psia. No N2, CO2, or H2S.
Step 1 — Pseudocritical (Sutton):
Tpc = 169.2 + 349.5*0.65 - 74.0*0.65^2 = 169.2 + 227.2 - 31.3 = 365.1 deg R
Ppc = 756.8 - 131.0*0.65 - 3.6*0.65^2 = 756.8 - 85.2 - 1.5 = 670.1 psia
Step 2 — Reduced T, P:
Tpr = 710 / 365.1 = 1.94
Ppr = 4000 / 670.1 = 5.97
Step 3 — Z-factor (Hall-Yarborough):
Z ~ 0.876 (from iteration at Tpr = 1.94, Ppr = 5.97)
Step 4 — Gas density:
M = 28.96 * 0.65 = 18.82 lb/lbmol
rho_g = (4000 * 18.82) / (0.876 * 10.732 * 710)
= 75280 / 6672
= 11.28 lb/ft^3
= 0.1807 g/ccStep 5 — LGE viscosity:
K = (9.4 + 0.02*18.82) * 710^1.5 / (209 + 19*18.82 + 710)
= (9.4 + 0.38) * 18914 / (209 + 357.6 + 710)
= 9.78 * 18914 / 1276.6
= 144.9
X = 3.5 + 986/710 + 0.01*18.82 = 3.5 + 1.389 + 0.188 = 5.08
Y = 2.4 - 0.2*5.08 = 1.38
mu_g = 1e-4 * 144.9 * exp(5.08 * 0.1807^1.38)
= 0.01449 * exp(5.08 * 0.0930)
= 0.01449 * exp(0.472)
= 0.01449 * 1.604
= 0.0232 cpValid Ranges
| Parameter | Method | Valid Range |
|---|---|---|
| Viscosity | LGE 1966 | P = 100–8000 psia, T = 100–340 °F, sg = 0.55–1.85 |
| Pseudocritical | Sutton | sg = 0.55–1.85, hydrocarbon-dominated |
| Wichert-Aziz | sour gas | yCO2 ≤ 0.80, yH2S ≤ 0.74 |
| Hall-Yarborough Z | Z-factor | Tpr > 1.0, Ppr = 0.1–15 |
| CKB impurity | sour viscosity | yN2 ≤ 0.15, yCO2 ≤ 0.15, yH2S ≤ 0.15 |
When the correlations do not apply
- Very rich gas condensates (sg > 1.85) — LGE drifts; use a tuned EOS PVT model.
- Highly sour systems (yH2S > 0.30) — Wichert-Aziz envelope ends, use measured lab data or tuned EOS.
- Near-critical or retrograde behavior — correlation outputs become unreliable; use a Peng-Robinson or SRK EOS.
- CCUS injection streams (pure or near-pure CO2) — use Fenghour-Wakeham CO2 viscosity correlation, not LGE.
References
- Lee, A.L., Gonzalez, M.H., & Eakin, B.E. (1966). "The Viscosity of Natural Gases." JPT, 18(8), 997–1000.
- Carr, N.L., Kobayashi, R., & Burrows, D.B. (1954). "Viscosity of Hydrocarbon Gases Under Pressure." Trans. AIME, 201, 264–272.
- Wichert, E. & Aziz, K. (1972). "Calculate Z's for Sour Gases." Hydrocarbon Processing, 51(5), 119–122.
- Hall, K.R. & Yarborough, L. (1973). "A New Equation of State for Z-Factor Calculations." Oil and Gas Journal, June 18, 82–92.
- Dranchuk, P.M. & Abou-Kassem, J.H. (1975). "Calculation of Z Factors for Natural Gases Using Equations of State." J. Canadian Petroleum Technology, 14(3), 34–36.
- Sutton, R.P. (1985). "Compressibility Factors for High-Molecular-Weight Reservoir Gases." SPE 14265.
- McCain, W.D. Jr. (1990). The Properties of Petroleum Fluids, 2nd ed. PennWell. Chapter 6.
- GPSA Engineering Data Book, 13th ed., Section 23 (Physical Properties).