Overview
Nodal analysis (systems analysis) is a method for optimizing well performance by dividing the production system into inflow (reservoir to node) and outflow (node to surface) components and finding the intersection point — the operating point. Developed by Gilbert (1954) and systematized by Brown (1977), it is the foundation of production optimization, artificial lift selection, and completion design.
Theory
The production system from reservoir to separator can be analyzed at any "node" (typically the bottomhole). At the node:
- Inflow: Reservoir delivers fluid to the node (IPR curve)
- Outflow: Tubing/flowline moves fluid from the node to surface (VLP/TPC curve)
The operating point is where inflow = outflow (supply = demand). Changing any component (tubing size, choke, reservoir pressure, artificial lift) shifts the curves and changes the operating point.
Formulas
Inflow Performance (IPR)
Vogel (below Pb):
q/qmax = 1 - 0.2*(Pwf/Pr) - 0.8*(Pwf/Pr)^2
Darcy (above Pb):
q = J * (Pr - Pwf)
Outflow Performance (VLP — Vertical Lift Performance)
The VLP curve is calculated using multiphase flow correlations (Beggs-Brill, Hagedorn-Brown, or Gray) from wellhead to bottomhole:
Pwf_required = WHP + ΔP_gravity + ΔP_friction - ΔP_acceleration
For single-phase liquid (simplified):
Pwf = WHP + 0.433 * SG * L + f * ρ * v^2 * L / (2 * D)
Operating Point
Solve simultaneously:
q_IPR(Pwf) = q_VLP(Pwf)
Graphically: intersection of IPR and VLP curves.
System Sensitivity Analysis
Common nodal analysis sensitivities:
- Tubing size: Larger tubing → lower friction → shifts VLP left → higher rate (up to a point where slip increases)
- WHP: Higher backpressure → shifts VLP up → lower rate
- Reservoir depletion: Lower Pr → shifts IPR down → lower rate
- GLR: Gas lift changes VLP shape — optimum GLR minimizes VLP
- Water cut: Increases hydrostatic head → shifts VLP up
- Brown, K.E. & Beggs, H.D. (1977). The Technology of Artificial Lift Methods, Vol. 1. PennWell.
- Gilbert, W.E. (1954). "Flowing and Gas-Lift Well Performance." Drilling and Production Practice, API.
- Golan, M. & Whitson, C.H. (1991). Well Performance, 2nd ed. Prentice Hall.
- PetroWiki — Nodal analysis: https://petrowiki.spe.org/Nodal_analysis
Critical Velocity (Turner Equation for Gas Wells)
v_critical = 1.593 * σ^0.25 * ρL^0.25 / ρG^0.5 (ft/s)
Below critical velocity, liquid loading occurs and well may die.
Worked Example
Given: Pr = 3,500 psi, Pb = 2,800 psi, J = 2.0 STB/d/psi (above Pb), WHP = 200 psi, 2-7/8" tubing, depth = 7,000 ft, SG = 0.85, GLR = 500 scf/STB.
Inflow (Composite IPR):
At Pwf = 2,800 psi: q = 2.0 * (3,500 - 2,800) = 1,400 STB/d
qmax_vogel = 1,400 + J*Pb/1.8 = 1,400 + 3,111 = 4,511 STB/d
At Pwf = 2,000 psi:
q_vogel_below = 3,111 * (1 - 0.2*(2000/2800) - 0.8*(2000/2800)^2)
= 3,111 * (1 - 0.143 - 0.408) = 3,111 * 0.449 = 1,397
q_total = 1,400 + 1,397 = 2,797 STB/dOutflow (VLP): Calculated using Beggs-Brill or correlation — produces a curve of Pwf_required vs q.
Operating point: Where IPR crosses VLP, e.g., q ≈ 2,200 STB/d at Pwf ≈ 2,200 psi.
Key Design Variables
| Component | Effect on Operating Point |
|---|---|
| Tubing ID increase | Lowers VLP → higher rate (to a limit) |
| WHP increase | Raises VLP → lower rate |
| Gas lift | Lowers VLP (lighter column) → higher rate |
| ESP | Adds ΔP to IPR side → dramatically higher rate |
| Reservoir depletion | Lowers IPR → lower rate over time |
| Skin damage | Shifts IPR left → lower rate |