(48)
∂H/∂gμν = -Γμβα Γναβ
∂H/∂gσμν = Γμνσ
If we now carry out the variations in (47a), we obtain the system of equations
(47b) ∂/∂xα ( ∂H/∂gαμν ) - ∂H/∂gμν = 0,
which, owing to the relations (48), coincide with (47), as was required to be proved.
If (47b) is multiplied by gσμν, since
∂gσμν/∂xα = ∂gαμν/∂xσ
and consequently
gσμν ∂/∂xα (∂H/∂gαμν) = ∂/∂xα (gσμν ∂H/∂gαμν)