A 12 kg block is pushed up a rough plane inclined at 37° by a horizontal force of 200 N. If the coefficient of friction is 0.20 and $\sin 37^\circ = 0.6$, $\cos 37^\circ = 0.8$, and $g = 10\,\text{m/s}^2$, what is the acceleration of the block?
The acceleration is $a \approx 3.7\,\text{m/s}^2$ up the plane. Along the plane, the driving component is $200\cos 37^\circ = 160\,\text{N}$, while the opposing forces are $mg\sin 37^\circ = 72\,\text{N}$ and friction $\mu N = 0.2( mg\cos 37^\circ + 200\sin 37^\circ ) = 43.2\,\text{N}$. The net force is $160 - 72 - 43.2 = 44.8\,\text{N}$, so $a = 44.8/12 \approx 3.73\,\text{m/s}^2$.
What you need to do here
Because the applied force is horizontal, it has one component up the slope and another component pushing the block into the slope. That second component increases the normal reaction, which increases friction, so we must compute $N$ before using $f=\mu N$.
Resolve the 200 N horizontal force relative to the plane
The plane makes angle $\theta = 37^\circ$ with the horizontal, so the horizontal force makes angle $\theta$ with the plane.
- Component up the plane: $$F_{\parallel} = 200\cos\theta = 200(0.8)=160\,\text{N}$$
- Component into the plane: $$F_{\perp} = 200\sin\theta = 200(0.6)=120\,\text{N}$$
Weight components
With $m=12\,\text{kg}$ and $g=10\,\text{m/s}^2$, $mg=120\,\text{N}$.
- Down the plane: $$mg\sin\theta = 120(0.6)=72\,\text{N}$$
- Into the plane: $$mg\cos\theta = 120(0.8)=96\,\text{N}$$
Normal reaction and friction
The normal reaction balances the total force into the plane: $$N = mg\cos\theta + F_{\perp} = 96 + 120 = 216\,\text{N}$$
Friction opposes the motion (block is pushed up, so friction acts down): $$f = \mu N = 0.20(216)=43.2\,\text{N}$$
Net force up the plane and acceleration
Take up the plane as positive: $$F_{\text{net}} = 160 - 72 - 43.2 = 44.8\,\text{N}$$
Then $$a = \frac{F_{\text{net}}}{m} = \frac{44.8}{12} = 3.73\,\text{m/s}^2$$
So the block accelerates at about $3.7\,\text{m/s}^2$ up the plane.
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