
To determine the thermal conductivity of the composite rod made of two rods A and B of different materials, we consider the configuration as two rods in parallel because both are welded together and will conduct heat simultaneously. The concept of effective thermal conductivity for composite materials in parallel can be applied here.
When two materials are arranged in parallel with thermal conductivities \( K_1 \) and \( K_2 \), the effective thermal conductivity \( K_{\text{eff}} \) of the composite is given by:
K_{\text{eff}} = \frac{K_1 + K_2}{2}
Here, the assumption is that both rods have the same cross-sectional area, and they receive the same temperature difference across their length. This results in the average of the two conductivities as the effective conductivity for the composite in a parallel configuration.
Thus, the effective thermal conductivity of the composite rod is:
\(\frac{K_1 + K_2}{2}\)
This makes option \(\frac{K_1 + K_2}{2}\) correct.
Three identical heat conducting rods are connected in series as shown in the figure. The rods on the sides have thermal conductivity 2K while that in the middle has thermal conductivity K. The left end of the combination is maintained at temperature 3T and the right end at T. The rods are thermally insulated from outside. In steady state, temperature at the left junction is \(T_1\) and that at the right junction is \(T_2\). The ratio \(T_1 / T_2\) is 
Calculate the \(E^\circ_{{Mg^{2+}/Mg}}\) potential for the following half-cell at 25°C:
Mg/Mg2+(1 × 10−4 M), E0 Mg2+/Mg = +2.36 V