Daniel B. answered 05/24/21
A retired computer professional to teach math, physics
Let
v = 60 km/h = 50/3 m/s be his speed at the bottom,
s = 75 m be the length of the hill,
α be the angle of the hill,
tan(α) = 0.08,
f = 0.1 be the coefficient of friction,
m be his mass (including equipment),
g = 9.81 m/s2 be gravitational acceleration,
h = sin(α)s be the height of the hill,
P = mgh be his potential energy at the top,
K = mv²/2 be his kinetic energy at the bottom,
F = mgcos(α) be the component of his weight normal to the slope,
W = Ffs be the work performed by friction on his way to the top.
To get up the hill, his kinetic energy at the bottom must be enough
for his potential energy at the top plus the work of friction.
K ≥ P + W
mv²/2 ≥ mgsin(α)s + mgcos(α)fs
v²/2 ≥ gsin(α)s + gcos(α)fs
v²/2 ≥ gs(tan(α) + f)cos(α)
v²/2gs(tan(α) + f) ≥ cos(α)
Substituting actual numbers
(50/3)²/(2×9.81×75×(0.08+0.1)) ≥ cos(α)
1.04 ≥ cos(α)
That inequality is always satisfied without having to calculate cos(α).
Therefore he will make it up the hill.