Step 1: Derive the factor of 3 from first principles instead of quoting $\Delta V/V = 3\alpha\Delta T$ directly.
Think of a small cube of the rod's material with edge $L$. When heated by $\Delta T$, each of its three edges, length, width and height, expands by the same linear factor:
\[ L' = L(1+\alpha\Delta T) \]
Step 2: Cube this to get the new volume.
\[ V' = (L')^3 = L^3(1+\alpha\Delta T)^3 \]
Expanding $(1+\alpha\Delta T)^3$ with the binomial expansion and dropping the tiny squared and cubed terms, since $\alpha\Delta T$ is extremely small:
\[ (1+\alpha\Delta T)^3 \approx 1 + 3\alpha\Delta T \]
Step 3: Read off the fractional change in volume.
\[ \frac{V'-V}{V} = \frac{\Delta V}{V} \approx 3\alpha\Delta T \]
This shows directly why the factor of 3 appears, one contribution from each of the three dimensions expanding together.
Step 4: Substitute the given numbers.
\[ \alpha = 10\times10^{-6} \ ^{\circ}\text{C}^{-1}, \quad \Delta T = 10 \ ^{\circ}\text{C} \]
\[ \frac{\Delta V}{V} = 3 \times 10\times10^{-6} \times 10 = 3\times10^{-4} \]
Step 5: Convert to a percentage.
\[ 3\times10^{-4} \times 100 = 0.03\% \]
Final Answer:
\[ \boxed{0.03\%} \]