Answer:

Step-by-step explanation:
Given:
- temperature at one end of the rod,

- temperature at the other end of the rod,

- amount of heat transferred in the first case,

- let initial length of the rod be,

- length of the rod in second case,

Using Fourier's law of conduction:

where:
k = thermal conductivity of the material
A = cross-sectional area normal to the direction of temperature change
dT = temperature difference
L = length across the surfaces of temperature difference
Now, when the rod is stretched to twice its length then its area becomes half because its volume remains constant.
Hence Fourier's law becomes:

the new rate of heat transfer is
