๐ŸงŠ Linde-Hampson Gas Liquefaction

Analyze the Linde-Hampson cycle for gas liquefaction using Joule-Thomson expansion with counter-flow heat exchange. Compute liquid yield, compressor work, COP, and figure of merit.

๐Ÿ“ Configuration

๐Ÿงช Gas Selection
๐ŸŒก๏ธ Operating Conditions
Set = Tin for no external pre-cooling
โš™๏ธ Compressor
Key Equations:

y = (hโ‚ โˆ’ hโ‚‚) / (hโ‚ โˆ’ h_f) โ€” liquid yield
W_comp = RยทTยทln(Pโ‚‚/Pโ‚) / ฮทc
W_liq = W_comp / y
COP = h_fg / W_liq
ฮผ_JT = (1/c_p)(2a/RT โˆ’ b)

๐Ÿ“Š Results

Configure inputs and click Analyze to view results.

๐Ÿ“˜ Methodology

Linde-Hampson Cycle

The Linde cycle uses isothermal compression followed by JT expansion to liquefy gases. A counter-flow heat exchanger pre-cools the high-pressure stream using the cold returning gas, progressively lowering temperatures until liquefaction occurs.

Yield & Make-up

The liquid fraction y represents the fraction of compressed gas that is liquefied per pass. The unliquefied gas returns through the HX, and fresh make-up gas compensates for the liquid withdrawn. Higher pressure increases yield but also compressor work.

Limitations

  • Requires Tin < Tinv for JT cooling.
  • Hydrogen and helium need pre-cooling below their Tinv.
  • Van der Waals model is approximate; more accurate EOS (Peng-Robinson, SRK) improve predictions.
  • Real HX has finite effectiveness.