Step 1: Understanding the Concept:
When a source moves toward a stationary observer, the observed frequency increases because the wavefronts are compressed.
Step 2: Formula:
\[ f' = f\cdot\frac{v}{v - v_s} \]
Step 3: Compute:
\[ f' = 450\times\frac{340}{340 - 34} = 450\times\frac{340}{306} = 450\times\frac{10}{9} = 500 \text{ Hz} \]
Step 4: Why the other options are wrong.
440 Hz is lower than the source frequency, which would be heard if the train were moving away. 480 Hz and 540 Hz do not match \(\frac{340}{306}\), and 540 Hz would be \(450\times1.2\).
Final Answer:
The frequency heard is \(500\) Hz, option (C).
\[ \boxed{500\text{ Hz}} \]