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Oil & Gas · Professional Microtool

Pipeline Pressure Drop Calculator

Outlet pressure · Velocity · Erosional limit

Outlet pressure along a gas pipeline from the isothermal flow equation, with the friction factor taken from the flow itself and the acceleration term solved by iteration rather than dropped.

9 inputs Screening estimate for hydraulic checks and capacity questions No registration Nothing you enter leaves your browser

Length Bore Inlet Velocity out Outlet Pressure drop along the run

Start from an example: 100 MMSCFD through 100 km of 590 mm line at 70 bar a →

Flow

Throughput at standard or contract conditions.

Pipeline

Length of the segment between the two pressure points, with no station in between.

Actual bore, not the nominal size. Capacity scales close to the two-and-a-half power of it.

About 0.0457 mm (1.8 mil) for new internally coated steel; bare or aged pipe is several times rougher.

Operating conditions

Absolute pressure at the start of the segment.

Average gas temperature along the segment. Buried lines settle close to ground temperature within a few kilometres of the station.

Gas properties

About 18.5 for lean natural gas. Heavier gas is denser and costs more pressure for the same standard volume.

Average Z along the segment. Around 0.85–0.92 at transmission pressures.

About 1.1 × 10⁻⁵ Pa·s for natural gas at transmission conditions. It only enters through the Reynolds number, so the answer is insensitive to it.

Full output

  • Pressure drop
  • Drop as a share of inlet
  • Drop per kilometre
  • Velocity at outlet
  • Erosional limit at outlet
  • Velocity at inlet
  • Mass flow
  • Reynolds number
  • Friction factor

Outlet pressure against throughput

Pressure enters the equation squared, so the curve falls away faster and faster: doubling throughput costs roughly four times the drop, which is why a line that looks comfortable today runs out of capacity abruptly rather than gradually.

Keep it

Both carry the figures you entered, in the part of the address that is never sent to a server. Share only where that is appropriate. To keep a copy for a project file, print the page — it lays itself out as a document.

Need a production-ready pipeline model?

We can extend this calculation to real elevation, compressor stations, operating telemetry and your actual pipeline data.

Discuss your use case →

Calculation basis 5 steps · view the method →
  1. Mass flow = standard flow × density at 0 °C and 101.325 kPa
  2. Reynolds number = mass flux × diameter ÷ viscosity
  3. Friction factor from Swamee-Jain on that Reynolds number and the relative roughness
  4. P₁² − P₂² = G²·Z·R·T·(f·L/D + 2·ln(P₁/P₂)), solved for P₂ by iteration
  5. Velocity at the outlet, where the gas is least dense and therefore fastest
Assumptions & limitations Screening estimate for hydraulic checks and capacity questions · 8 assumptions →

This is a screening calculation for steady, isothermal, single-phase gas in a horizontal line of constant bore. It excludes elevation change, liquid holdup and two-phase flow, heat transfer with the ground, fittings and valves, compressor station effects, transient and packing behaviour, and any real-gas treatment beyond a single Z. Design, rating and regulatory work require a proper hydraulic model and the applicable pipeline code — this figure is for orientation only.

  • Steady, isothermal, single-phase gas flow in a horizontal line of constant internal diameter.
  • Elevation change is ignored, which matters on hilly terrain and for dense gas.
  • Liquid holdup and two-phase behaviour are not modelled; any condensate changes the answer substantially.
  • Gas properties — Z, molecular weight and viscosity — are taken as constant along the segment.
  • Fittings, valves, bends, station piping and metering losses are excluded.
  • The erosional velocity uses API RP 14E with C = 100 in field units, a rule of thumb rather than a limit derived for your service.
  • Transient and line-pack behaviour is out of scope: this is a steady-state answer.
  • Where the flow cannot be carried from the given inlet pressure, the tool reports that there is no steady-state solution rather than an outlet of zero — and near sonic conditions this model stops being applicable well before that point.

Worked examples

About this tool

Pipeline hydraulics is where a screening number is most useful and most often taken too far. This tool runs the isothermal flow equation properly — friction from the actual Reynolds number, the expansion term solved rather than assumed away — and reports the velocity against the erosional limit, which is the check that decides whether a line is workable at all. Written for pipeline, facilities and process engineers.

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