Light-rail passenger trains that provide transportation within and between cities are capable of modest accelerations. The magnitude of the maximum acceleration is typically 1.3 {\rm m}/{\rm s}^{2}, but the driver will usually maintain a constant acceleration that is less than the maximum. A train travels through a congested part of town at 4.0m/s . Once free of this area, it speeds up to 11m/s in 8.0 {\rm s}. At the edge of town, the driver again accelerates, with the same acceleration, for another 16 {\rm s} to reach a higher cruising speed.

What is the questi0n?

What is the final speed?

38

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To solve this problem, we need to find the acceleration of the train when it speeds up to reach 11 m/s in 8.0 s, as well as the acceleration when it reaches its cruising speed.

Let's start with the first part of the problem. The train initially travels at 4.0 m/s and speeds up to 11 m/s in 8.0 s.
We can use the following kinematic equation to find the acceleration:
vf = vi + at
where:
vf is the final velocity (11 m/s),
vi is the initial velocity (4.0 m/s),
a is the acceleration, and
t is the time (8.0 s).

Rearranging the equation to solve for the acceleration (a), we get:
a = (vf - vi) / t

Substituting the given values, we have:
a = (11 m/s - 4.0 m/s) / 8.0 s

Simplifying the equation, we get:
a = 7.0 m/s / 8.0 s
a = 0.875 m/s^2

So, the acceleration of the train when it speeds up to reach 11 m/s in 8.0 s is 0.875 m/s^2.

Now let's move on to the second part of the problem. The train accelerates for another 16 s to reach its cruising speed.
Given that the magnitude of the maximum acceleration is typically 1.3 m/s^2, we can assume that the acceleration during this phase is also 1.3 m/s^2.

Therefore, the acceleration of the train when it reaches its cruising speed is 1.3 m/s^2.

To summarize:
- The acceleration of the train when it speeds up to reach 11 m/s in 8.0 s is 0.875 m/s^2.
- The acceleration of the train when it reaches its cruising speed is 1.3 m/s^2.