To solve this problem, we can use the kinematic equation:
vf^2 = vi^2 + 2aΔx
Where:
vf = final velocity (0 m/s, since the car comes to rest)
vi = initial velocity (40.0 m/s)
a = constant acceleration
Δx = displacement (200 m)
Plugging in the values, we get:
(0 m/s)^2 = (40.0 m/s)^2 + 2a(200 m)
0 = 1600 m^2/s^2 + 400a
Rearranging the equation, we find:
400a = -1600 m^2/s^2
Dividing both sides by 400:
a = -4.0 m/s^2
Therefore, the constant acceleration of the car after the brakes are applied must be -4.0 m/s^2. Note that the negative sign indicates that the acceleration is opposite to the initial velocity, which is required for the car to come to rest.