Step 1: Treat each rod like a resistor
Heat flow behaves like current. A rod of length $L$, area $A$ and conductivity $k$ has thermal resistance $R_{th}=\frac{L}{kA}$. The temperature difference plays the role of voltage.
Step 2: Add the resistances in series
Let $R=\frac{L}{KA}$. The outer rods have $\frac{R}{2}$ each and the middle rod has $R$. Total resistance is $\frac{R}{2}+R+\frac{R}{2}=2R$.
Step 3: Find the heat current
The total temperature drop is $3T-T=2T$. So the heat current is $H=\frac{2T}{2R}=\frac{T}{R}$. The same $H$ flows through every rod because there is no side loss.
Step 4: Find the junction temperatures
Drop across the left rod: $H\cdot\frac{R}{2}=\frac{T}{2}$. So $T_1=3T-\frac{T}{2}=\frac{5T}{2}$. Drop across the middle rod: $H\cdot R=T$. So $T_2=T_1-T=\frac{3T}{2}$. Check with the right rod: $T_2-\frac{T}{2}=T$, which matches the cold end.
Step 5: Compare with the options
$\frac{T_1}{T_2}=\frac{5}{3}$. The values $\frac{3}{2}$, $\frac{4}{3}$ and $\frac{4}{5}$ do not match these temperatures, so they are rejected.
Final Answer:
Using the thermal resistance method, the ratio is 5/3.
\[ \boxed{\dfrac{5}{3}\ \text{(C)}} \]