Given that the rod is of circular cross-section and tapered uniformly, and assuming steady-state heat conduction with no internal heat generation, the total heat flow (Q) through any cross-section remains constant.
Heat flux ($q$) is defined as:
\[
q = \frac{Q}{A}
\]
So if $Q$ is constant, then:
\[
q \propto \frac{1}{A}
\Rightarrow q \propto \frac{1}{\pi d^2/4} \Rightarrow q \propto \frac{1}{d^2}
\]
Let $q_1$ be the heat flux at the larger end ($d_1 = 5$ cm), and $q_2$ be the heat flux at the smaller end ($d_2 = 2.5$ cm):
\[
\frac{q_2}{q_1} = \left( \frac{d_1}{d_2} \right)^2 = \left( \frac{5}{2.5} \right)^2 = 2^2 = 4
\Rightarrow q_2 = 4 \cdot q_1 = 4 \cdot 2500 = 10,000 \ \text{kcal/m}^2\cdot\text{hr}
\]
Thus, the heat flux at the smaller end is 10,000 kcal/m$^2\cdot$hr.