Enthalpy of a mixture of gases is determined by this formula:
$$h=\Sigma (mf)_ih_i\;[\mathrm {kJ/kg}]$$
$h$ is the enthalpy of unit mass of the mixture,
$(mf)_i$ is mass fraction of gas $i$, $(mf)_i=\large{\frac{m_i}m}$ ($m_i$ is the mass of gas $i$ and $m$ is the mass of mixture)
$h_i$ is the enthalpy of unit mass of gas $i$ that can be determined by using $\textrm{one}^1$ of Dalton's law of additive pressures or Amagat's law of additive volumes and temperature of the mixture.
In this case, if we assume that $\large{\frac{m_v}{m_a}}=\mu$; as $m=m_v+m_a$, then we have
$$(mf)_v=\large{\frac{\mu}{\mu+1}}$$
and
$$(mf)_a=\large{\frac 1{\mu+1}}$$
Thus,
$$\large{h}=\large{\frac{\mu}{\mu+1}}h_v+\large{\frac 1{\mu+1}}h_a$$
$^{\mathrm 1}$ For mixture of ideal gases, both of these laws end to same result, but for mixture of real gases, choosing between these two laws depends on the problem.