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