Crate on a frictionless ramp, constant speed.

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Homework Help Overview

The problem involves a 130 kg crate being pushed at constant speed up a frictionless ramp inclined at 23°. Participants are discussing the forces acting on the crate, particularly focusing on the horizontal force required to maintain constant speed against gravitational forces.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the relationship between the gravitational force acting on the crate and the applied horizontal force. There are attempts to express the forces mathematically and questions about the components of these forces in relation to the incline.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of force components and their relationships. Some guidance has been offered regarding the need to consider the horizontal and parallel components of forces, but no consensus has been reached on the final calculations.

Contextual Notes

Participants are navigating the complexities of force components in a frictionless scenario, with some expressing confusion about the application of trigonometric relationships and the role of the normal force.

Koscher
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Homework Statement



A 130 kg crate is pushed at constant speed up the frictionless 23° ramp shown in the figure. What horizontal force F is required?

Homework Equations



F=ma
F(parallel)=mgsin(theta)
F(perpendicular)=mgcos(theta)

The Attempt at a Solution



I know that because it is at a constant speed the net force equals zero, therefore the force caused by gravity equals the applied force. So first I solved the parallel force caused by gravity, which equals 498.2994 N. From there to create a net force of zero I flipped the sign, -498.2994 N. Solved for the horizontal component of that force: -498.2994cos23 =-458.687 N.

But obviously that was not right. I think I might have to include the normal force by gravity in that equation too though. Any thoughts?
 
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Koscher said:
I know that because it is at a constant speed the net force equals zero, therefore the force caused by gravity equals the applied force. So first I solved the parallel force caused by gravity, which equals 498.2994 N. From there to create a net force of zero I flipped the sign, -498.2994 N. Solved for the horizontal component of that force: -498.2994cos23 =-458.687 N.
Since the applied force is horizontal, you have found the component of F parallel to the incline. Now you need to find the full force F. Express that mathematically so you can solve for F.
 
I am afraid that I am a little lost at the moment. I need to express the full force of the equation?
 
If the applied force F is horizontal, what would be its component parallel to the incline?
 
Force applied(parallel) = Force applied(sin(theta))

So: 498.2994/sin(23) = 1275.3 N [force applied]
 
Koscher said:
Force applied(parallel) = Force applied(sin(theta))
Not exactly. Realize that the applied force is horizontal, not vertical (like gravity).
 
Okay so the applied force in the direction of parallel, would that be an equal but opposite force to the force parallel caused by the force of gravity?
 
Koscher said:
Okay so the applied force in the direction of parallel, would that be an equal but opposite force to the force parallel caused by the force of gravity?
Yes, if I understand what you mean. The net force in any direction must be zero. Thus the forces parallel to the ramp must be zero. Thus the parallel component of gravity and the parallel component of the applied force must be equal and opposite.
 
Okay.

If I take the horizontal component of the Normal force and the horizontal component of the applied force and add them together, will that give me a total horizontal force.

(498.299cos23)=458.6866 N
(1380sin23)=539.208 N

So, 997.8946 N?
 
  • #10
Koscher said:
If I take the horizontal component of the Normal force and the horizontal component of the applied force and add them together, will that give me a total horizontal force.
Since the crate is in equilibrium, the net horizontal force will be zero. Some problems with this approach:
- The applied force is totally horizontal, so the horizontal component of the applied force is the applied force
- The normal force does not simply equal mgcosθ

You'll have a much easier time if you stick to the force components parallel to the ramp.
 
  • #11
Okay.

So.

Fcos(theta)-mgsin(theta)=ma
Fcos(23)-(130kg)(9.81 m/s^2)sin(23)=0 (it equals zero because of the zero net force)

Solve for F.

F= 541.332 N

Sorry for being a pain, I have been fine with similar questions, just this one was confusing. You were a huge help, thank you. That would be the answer if I am not mistaken.
 
  • #12
Good!
 

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