Let KA and KB be the thermal conductivity of material A and B, respectively. Let T1 be the temperature of A and T2 be the temperature of B. At steady state, rate of flow of heat is given by,
ΔQ
Δt
=
ΔQA
Δt
=
ΔQB
Δt
⇒
K′A(T2−T1)
lA+lB
=
KAA(T−T1)
lA
=
KBA(T2−T)
lB
...(i) where K is thermal conductivity of both material and A and l are area and length of the material respectively. Using Eq. (i), we get
KAA
lA
(T−T1)=
KBA(T2−T)
lB
⇒ 2KB(T−T1)=KB(T2−T)(∵lA=lB and KA=2KB) ⇒ 2T−2T1=T2−T ⇒ 3T=T2+2T1 ⇒T=