Energy Problems of box acceleration

In summary, the work done by the applied force of 132.853 N on a 29.4 kg box pushed 3.5 m along a rough, horizontal floor is 1275.667 J, taking into account the force of kinetic friction with a coefficient of 0.408.
  • #1
JassC
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A 29.4 kg box initially at rest is pushed 3.5 m along a rough, horizontal floor with a constant applied horizontal force of 132.853 N. The acceleration of gravity is 9.8 m/s^2 . If the coefficient of friction between box and floor is 0.408, find the work done by the applied force. Answer in units of J.

My understanding that it is asking for the applied force WITHOUT the friction? So just 3.5m * (29.4kg)(9.8m/s^2) = the applied force?
 
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  • #2
JassC said:
A 29.4 kg box initially at rest is pushed 3.5 m along a rough, horizontal floor with a constant applied horizontal force of 132.853 N. The acceleration of gravity is 9.8 m/s^2 . If the coefficient of friction between box and floor is 0.408, find the work done by the applied force. Answer in units of J.

My understanding that it is asking for the applied force WITHOUT the friction? So just 3.5m * (29.4kg)(9.8m/s^2) = the applied force?
You may wish to reconsider your answer there, what is the definition of work done?
 
  • #3
Expanding Hootenanny's hint:

[tex]W = \Sigma \vec{F} \times \Delta s[/tex]

and

[tex]\Sigma \vec{F} = F - F_{a}[/tex]

[tex]F[/tex] - constant applied horizontal force of 132.853 N
 
  • #4
Sorry.

But that didn't help me :(
 
  • #5
JassC said:
Sorry.

But that didn't help me :(

OK. No problem. :smile:

[tex]\Sigma \vec{F} = F - f_k[/tex]

[tex]F[/tex] - constant applied horizontal force of 132.853 N
[tex]f_k[/tex] - force of kinetic friction

To find the kinetic friction force:

[tex]f_k =\mu_k.n[/tex]
where [itex]n[/itex] is the normal force, and since the box is along an horizontal floor it is equal to the weight of the box.

Then
, you calculate [itex]\Sigma \vec{F}[/itex], using [itex]\Sigma \vec{F} = F - f_k[/itex]

And finally, you compute the work done, using [itex]W = \Sigma \vec{F} \times \Delta s[/itex], since you now know [itex]\Sigma \vec{F}[/itex] and [itex]\Delta s[/itex].

I hope this time you understand. If not, we are here to provide more help. :wink:
 
  • #6
Alright I got the correct answer.

Thanks!
 

FAQ: Energy Problems of box acceleration

What is the concept of "Energy Problems of box acceleration"?

The concept of "Energy Problems of box acceleration" involves the study of how energy is conserved and transformed when a box is accelerated. This includes understanding the different types of energy involved, such as kinetic and potential energy, and how they change as the box moves.

What factors affect the energy problems of box acceleration?

The energy problems of box acceleration are affected by several factors, including the mass of the box, the initial velocity of the box, the external forces acting on the box, and the distance over which the box is accelerated. These factors can impact the amount of energy involved and how it is transformed.

How does the conservation of energy apply to box acceleration?

The law of conservation of energy states that energy cannot be created or destroyed, only transformed from one form to another. This applies to box acceleration as well, as the total amount of energy involved in the system (box, external forces, and surroundings) remains constant, even as the energy is transformed between kinetic and potential forms.

What are some real-world applications of energy problems of box acceleration?

The concept of energy problems of box acceleration has several real-world applications, such as in the design of roller coasters and other amusement park rides. It is also important in understanding the motion of objects in space, such as satellites and rockets, and in studying the impact of external forces on moving objects, such as in car crashes.

How can the energy problems of box acceleration be solved?

To solve energy problems of box acceleration, one must apply the principles of conservation of energy and Newton's laws of motion. This involves setting up and solving equations that relate the initial and final energies and velocities of the box, taking into account any external forces and the distance over which the box is accelerated. Calculating the work done by these forces can also help determine the final energy of the box.

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