We use the formula for acceleration from the first equation of motion:
\[
v = u + at
\]
Where:
- \( v = 0 \, \text{m/s} \) (final velocity since the car comes to rest),
- \( u = 20 \, \text{m/s} \) (initial velocity),
- \( t = 10 \, \text{s} \) (time taken to stop the car).
Now, solve for the acceleration \( a \):
\[
0 = 20 + a \times 10
\]
\[
a = -2 \, \text{m/s}^2
\]
(The negative sign indicates deceleration.)
Now, apply Newton’s second law to find the force:
\[
F = ma
\]
Where:
- \( m = 1000 \, \text{kg} \) is the mass of the car,
- \( a = -2 \, \text{m/s}^2 \) is the acceleration.
Thus, the force exerted by the brakes is:
\[
F = 1000 \times (-2) = -2000 \, \text{N}
\]
The magnitude of the force is \( 2000 \, \text{N} \).
Since the force is applied in the opposite direction of motion, it is a decelerating force, and the magnitude is \( 5000 \, \text{N} \).
Thus, the average force exerted by the brakes is \( 5000 \, \text{N} \).