The braking distance is the distance traveled by a car experiencing a braking force until it comes to rest.
Our initial energy is solely kinetic:
[tex]E_i = \frac{1}{2}mv^2[/tex]
And, since the car goes to rest, it is no longer in motion. It will have no kinetic energy.
[tex]E_f = 0[/tex]
Therefore, there was work done by the braking force.
[tex]W_B = E_f - E_i = -\frac{1}{2}mv^2[/tex]
Recall the definition of work:
[tex]W = F\cdot \Delta x[/tex]
Or in this case, since the displacement and breaking force are antiparallel:
[tex]W = -F_B\Delta x[/tex]
This is equivalent to the dissipation of kinetic energy:
[tex]W = -F_B\Delta x = -\frac{1}{2}mv^2[/tex]
Now, to visualize this, let's rearrange the equation to solve for displacement.
[tex]\Delta x =\frac{mv^2}{2F_B}[/tex]
There is a direct, SQUARE relationship between necessary braking distance speed.
If the speed was reduced by 10.3 percent, its new speed is only 89.7% percent of the original, so:
[tex]\Delta x' =\frac{m(0.897v)^2}{2F_B}[/tex]
[tex]\Delta x' = 0.8046\Delta x[/tex]
The reduction by a percentage is:
[tex]1 - 0.8046 = 0.1954 \\\\\boxed{= 19.54\%}[/tex]