A block slides without friction down a hill of height $h = 2$ m and then, passing smoothly onto a horizontal stretch, slides along it until it stops. The coefficient of friction on the horizontal stretch is $\mu = 0.25$ (see the figure). Find the speed of the block at the foot of the hill and the distance $s$ it travels along the horizontal stretch. Take $g = 10$ m/s².
There is no friction on the hill, so mechanical energy is conserved, while on the horizontal stretch all the kinetic energy goes into the work of friction. Compare three moments: $A$ — the top, $B$ — the foot, $C$ — the stop.
1. From $A$ to $B$ (energy is conserved):
$$mgh = \frac{mv^2}{2} \;\Rightarrow\; v = \sqrt{2gh} = \sqrt{2 \cdot 10 \cdot 2} = \sqrt{40} \approx 6.3 \text{ m/s}$$2. From $B$ to $C$ the kinetic energy turns completely into the work of friction $F_{fr} = \mu mg$ over the distance $s$:
$$\frac{mv^2}{2} = \mu mg\,s$$Or directly from $A$ to $C$: $mgh = \mu mg\,s$ — the mass cancels:
$$s = \frac{h}{\mu} = \frac{2}{0.25} = 8 \text{ m}$$$v \approx 6.3$ m/s; $s = 8$ m