To solve this problem it is necessary to apply the concepts related to
conservation of energy, for this case manifested through work and kinetic energy.
[tex]W = \Delta KE[/tex]
[tex]W = F*d[/tex]
Where,
F= Force (Frictional at this case [tex]F_r = \mu N[/tex])
d= Distance
[tex]\Delta KE = \frac{1}{2} mv^2[/tex]
Where,
m = mass
v = velocity
Equation both terms,
[tex]F*d = \frac{1}{2}mv^2[/tex]
[tex]\mu mg *d = \frac{1}{2}mv^2[/tex]
[tex]\mu g * d = \frac{1}{2}v^2[/tex]
[tex]d = \frac{1}{2} \frac{v^2}{\mu g}[/tex]
Replacing with our values we have that
[tex]d = \frac{1}{2} \frac{25^2}{0.65*9.8}[/tex]
[tex]d = 49.05m[/tex]
Therefore the shortest distance in which the truck can come to a halt without causing the crate to slip forward relative to the truck is 49.05m