To develop this problem we will apply the concept related to heat transfer defined as the product between the transfer coefficient and the temperature difference between two spaces, that is,
[tex]q=h(T_s-T_0)[/tex]
Here,
h = Heat transfer coefficient
[tex]T_{s,0}[/tex]= Temperature at each point
[tex]q = 5(20-16)[/tex]
[tex]q = 20 W/m^2[/tex]
[tex]q = 20(6-5)[/tex]
[tex]q = 20 W/m^2[/tex]
[tex]q = 5(16-20)[/tex]
[tex]q = -20 W/m^2[/tex]
We can see that the magnitude of the heat fluxes in the three states are the same (The negative sign only indicates the change of direction) so the wall is in steady state conditions