Joule-Brayton Process with Dry Air
- Using a more realistic medium:
- Dry Air = ideal gas with non-constant heat capacity cp(T)
- defined in MSL media library as DryAirNasa
- simply changing medium → model doesn't run
- inversion of h(T) with Dekker-Brent has wrong
start interval
- Problems with DryAirNasa:
- function for isentropic enthalpy uses constant cp
approximation
- provide better computation directly using
constant entropy
- compressor characteristics in ThermoDLR uses constant
cp
- inversion still gets wrong start interval
- problem: mass flow is zero initially
- use given mass flow as start value → model runs
- Finetuning:
- large deviations from expected results
- use procedure from Joule example above, including
simple test models
- internal inversions make model less stable
- fix: define ω instead of τ for compressor
- then closing circle and standard finetuning work