๐ŸŒ€ Throttling Valve & Joule-Thomson Effect

Analyze isenthalpic throttling processes. Compute the Joule-Thomson coefficient, outlet temperature, inversion temperature, and liquefaction feasibility using the van der Waals equation of state.

๐Ÿ“ Configuration

๐Ÿงช Gas Selection
โš—๏ธ Custom Gas Properties
๐ŸŒก๏ธ Operating Conditions
Must be less than Pin
Key Equations:

Isenthalpic: hin = hout
ฮผJT = (1/cp)(2a/RT โˆ’ b) [Van der Waals]
Tout = Tin + ฮผJTยทฮ”P
Tinv = 2a/(Rb) [max inversion temp]
Ideal gas: ฮผJT = 0

๐Ÿ“Š Results

Configure inputs and click Analyze to view results.

๐Ÿ“˜ Methodology

Isenthalpic Process

Throttling through a valve is isenthalpic (hin = hout) at steady state with negligible kinetic and potential energy changes. For a real gas, this causes a temperature change due to intermolecular forces.

Joule-Thomson Effect

The JT coefficient ฮผJT = (โˆ‚T/โˆ‚P)h determines whether throttling causes cooling (ฮผ>0) or heating (ฮผ<0). Most gases cool at room temperature; hydrogen and helium heat up because their inversion temperatures are very low.

Inversion Curve

The inversion temperature is where ฮผJT = 0. Below Tinv, the gas cools upon expansion. For the Van der Waals model: Tinv,max = 2a/(Rb). Gas liquefaction (Linde process) requires operating below Tinv.