f(t)/g(t) ≥ 2 for all mission times t ≥ 0.f'(t)=4t+175, g'(t)=2t+5f''(t)=4, g''(t)=2f''(t)/g''(t)=4/2=2 (constant)| t (hours) | f(t) | g(t) | f(t)/g(t) |
|---|---|---|---|
| 5 | 925 | 50 | 18.50 |
| 10 | 1,950 | 150 | 13.00 |
| 20 | 4,300 | 500 | 8.60 |
| 30 | 7,050 | 1,050 | 6.71 |
| 50 | 13,750 | 2,750 | 5.00 |
| t (hours) | Distance ratio f(t)/g(t) | Velocity ratio f'(t)/g'(t) |
|---|---|---|
| 240 | 2.67 | 2.34 |
| 720 | 2.23 | 2.11 |
| 1200 | 2.14 | 2.07 |
Conclusion: As t → ∞, both distance and velocity ratios approach 2.
f''/g'' = 2 forever, that’s the “target” long‑term ratio.f'(t)=4t+175 and g'(t)=2t+5 matter early, but become less important as t grows.Both probe distances grow without bound, but the ratio f(t)/g(t) drops toward 2 and never goes below it. The acceleration ratio is constant at 2, which forces the velocity ratio toward 2, and that forces the distance ratio toward 2. DiVA makes this “L’Hôpital idea” visible: each derivative step simplifies the long‑term comparison.
For same‑degree polynomials, the ratio approaches the ratio of the leading coefficients. In the provided challenge, that limiting ratio is 3.