Classic box up a hill problem

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In summary, we have a 10kg box being pushed up a 3m long hill at a 30 degree angle. We can assume no friction for questions a and b. To get the box to the top of the hill in 5.0s, it must have an acceleration of 0.24m/s2. The nett force on the box if it is accelerating at this rate is 86.07N. If the coefficient of kinetic friction between the box and the hill is 0.42, the force required to push the box is 51.4N.
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Ciricus
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Homework Statement


A 10kg Box is being pushed up a 3m long hill at the angle of 30 degrees. A constant force is being applied to the box parallel to the ramp. The box starts from rest. For questions a and b we can assume no friction.

a) If you were to get the box to the top of the hill in 5.0s, what acceleration must it have?

b) What is the nett force on the box if it is accelerating at this rate?

c) If the coefficient of kinetic friction between the box and the hill is 0.42, what force is required to push the box?

-----------------------------

2. Homework Equations (or so I believe)

a) d = Vit + [itex]\frac{1}{2}[/itex]at2

b) Fx = mgsin([itex]\Theta[/itex])
Fy= mgcos([itex]\Theta[/itex])

c) f =[itex]\mu[/itex]N

The Attempt at a Solution



a) d = Vit + [itex]\frac{1}{2}[/itex]at2
Since Vi = 0m/s d = [itex]\frac{1}{2}[/itex]at2

To solve for a: 2 [itex]\times[/itex] [itex]\left(\frac{d}{t^2}\right)[/itex]
a = 2 [itex]\times[/itex] [itex]\left(\frac{3m}{5s^2}\right)[/itex]
a = 0.24m/s2

b) x forces: Fx = mgsin([itex]\Theta[/itex])
Fx = mgsin(30)
Fx = 10kg [itex]\times[/itex] 0.24m/s2 [itex]\times[/itex] sin(30)
Fx = 1.2N

y forces: Fy = mgcos([itex]\Theta[/itex])
Fy = mgcos(30)
Fy = 10kg [itex]\times[/itex] 9.8m/s2 [itex]\times[/itex] cos(30)
Fy = 84.87N

[itex]\therefore[/itex] Nett force = Fx + Fy = 86.07N

-----------------------------

C) [itex]\mu[/itex] = [itex]\frac{f}{n}[/itex]
0.42 = [itex]\frac{f}{1.2}[/itex]
Which gives 0.5N

-----------------------------

I lost faith in my ability to do it after b). I'm not sure if you're supposed to be using 9.8m/s2 or 0.24m/s2 when finding the value for mgsin([itex]\Theta[/itex]). If i use 9.8m/s2 i get a more reasonable answer of 42N, however I'm not applying the 'new acceleration' into the equation at all.

Thanks for any help/direction with this in advance!
 
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  • #2
i think u should solve b as follows :
[itex]\sum[/itex]F=ma(here u need to use the acceleration)
F+W=ma
(F is the force u need to find and W is the force of gravity or weight)
projection along x-axis
f-Wx=ma ( -Wx because the force is acting in the opposite direction)
Wx=g.m.sin30=9.8[itex]\times[/itex]10[itex]\times[/itex]sin30=49N
THEN
F=Wx+ma=49+(10)(0.24)=51.4N
 
Last edited:

What is the "Classic box up a hill problem"?

The "Classic box up a hill problem" is a thought experiment that involves a box being pushed up a hill. It is often used in physics to illustrate concepts such as work, energy, and friction.

What are the main factors that affect the box's motion in this problem?

The main factors that affect the box's motion are the force applied to the box, the mass of the box, the angle of the hill, and the presence of friction.

How does the angle of the hill affect the motion of the box?

The steeper the hill, the more work is required to push the box up the hill. This is because the force of gravity acting against the box's motion increases as the angle of the hill increases.

How does friction play a role in this problem?

Friction is a force that opposes the motion of the box. It reduces the speed and increases the work required to push the box up the hill. The amount of friction depends on factors such as the surface of the hill and the weight of the box.

What is the relationship between work and energy in this problem?

The work done on the box is equal to the change in its kinetic energy. As the box is being pushed up the hill, its potential energy increases while its kinetic energy decreases. This relationship is described by the law of conservation of energy.

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