anchor.diff:          p \[ R = \frac{\hat{R}}{\hat{M}} \]
   
           h2#specific-heat-ratio Ratio of specific heats
  -        p \[ \gamma = \frac{C_p}{C_v} \]
  +        p \[ \gamma = \frac{c_p}{c_v} \]
           p \( \gamma = \frac{7}{5} \) for a diatomic gas, \( \gamma = \frac{5}{3} \) for a monotomic gas
       
       include ../inc/footer.jade
  
positive.code:             th Calorically Perfect Gas
            tr
              th Internal energy
              td \[ C_v = \left( \pddx{e}{T} \right)_p \]
              td \[ e = C_v T \]
            tr
              th Enthalpy
              td \[ C_p = \left( \pddx{h}{T} \right)_v \]
              td \[ h = C_p T \]
  
  
  
  
negative.code:         p \[ p = \rho R T \]
  
          h2#perfect-gas Perfect Gas
          p For a perfect gas, the specific heat capacity (\(c_v, c_p\)) is only temperature dependent, whereas it is constant for a calorically perfect gas.
          table
            tr
              th
  