Calculating Net Work on a Backpack on an Inclined Surface at Constant Velocity

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Homework Help Overview

The discussion revolves around calculating the net work done on a backpack being carried up an inclined surface at a constant velocity. The problem involves determining the work done by the hiker, the work done by gravity, and the net work, with a specific focus on the implications of constant velocity in the context of forces acting on the backpack.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the distinction between the work done by the hiker and the work done by gravity, questioning the directionality of these forces. Some participants suggest that gravity does negative work while the hiker does positive work, prompting discussions on the relationship between these forces when moving at constant velocity.

Discussion Status

There is an ongoing exploration of the concepts of work and force components, particularly regarding the incline and the vertical height. Some participants have offered clarifications about the calculations involved, while others are questioning the assumptions about the direction of forces and the nature of work done by gravity.

Contextual Notes

Participants note the importance of considering the incline's angle and the path taken when calculating work, as well as the implications of using components of forces in their calculations. The discussion reflects a mix of interpretations regarding the application of work-energy principles in this context.

MIA6
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Homework Statement


a) Determine the work a hiker must do on a 15.0-kg backpack to carry it up a hill of height h=10.0 m b) determine the work done by gravity on the backpack, and c)the net work done on the backpack. Assume the motion is at constant velocity.

I don't understand why the question asks you the work done by hiker and done by gravity. What's the difference? Is that the work done by hiker is in the direction of the motion, i mean the slope. However, the work done by gravity is in the direction of the altitude of the hill, height? On the book, the diagram is like a backpack, and then the force which points upward is the force by Hiker, the force points downward is the gravity. Hope you can clarify, thanks.
 
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Gravity doesn't actually do any work on the backpack because it is not moving downwards and you can't have a negative value for work. Work is only done when the object moves in the direction of the force being applied to it. Hope that helps.
 
XJellieBX said:
Gravity doesn't actually do any work on the backpack because it is not moving downwards and you can't have a negative value for work. Work is only done when the object moves in the direction of the force being applied to it. Hope that helps.

On my book, it finds the component of gravity which acts in the direction of motion, so it's not direct gravity, but the component.
 
XJellieBX said:
Gravity doesn't actually do any work on the backpack because it is not moving downwards and you can't have a negative value for work. Work is only done when the object moves in the direction of the force being applied to it. Hope that helps.
No, that's not right, the gravity force does do work, and since its direction is downward, and the backpack is moving upward, it does negative work. The hiker does positive work, since she must apply an upward lifting force on the backpack in the same direction as its vertical motion. Since the movement is at constant speed, what does this say about the relationship between the 2 forces and work done by each?
 
PhanthomJay said:
No, that's not right, the gravity force does do work, and since its direction is downward, and the backpack is moving upward, it does negative work. The hiker does positive work, since she must apply an upward lifting force on the backpack in the same direction as its vertical motion. Since the movement is at constant speed, what does this say about the relationship between the 2 forces and work done by each?

If I need to find the work done by hiker, W=Fd, so force is the upward force, but I think this force should be the component of the force exerted by the hiker, since the hiker climbs a slope which is some degree angle inclined to the ground; she is not climbing vertically. How about the force exerted by the gravity? Should I find the component of it, too? Why it is not in the direction of the height which is vertical but also that incline?
 
MIA6 said:
If I need to find the work done by hiker, W=Fd, so force is the upward force, but I think this force should be the component of the force exerted by the hiker, since the hiker climbs a slope which is some degree angle inclined to the ground; she is not climbing vertically. How about the force exerted by the gravity? Should I find the component of it, too? Why it is not in the direction of the height which is vertical but also that incline?
remember that work is not Fd it is Fdcostheta, that is, work is force times distance in the direction of the force. The gravity force is a conservative force such that the work done by gravity is independent of the path taken, so you just need to know the height in both cases.
 
PhanthomJay said:
remember that work is not Fd it is Fdcostheta, that is, work is force times distance in the direction of the force. The gravity force is a conservative force such that the work done by gravity is independent of the path taken, so you just need to know the height in both cases.

I know that a conservative force is independent of path it takes, but it starts down the ramp, and finishes up the ramp, so it's not the vertical distance, but between these two points?
 
Lets assume the ramp is sloped at 30 degrees with the horizontal (60 degrees with the vertical). The box, which weighs 150N, is raised to a height of 10m. This means that along the direction of the incline, it travels 20m, using basic trig. Since work is Fdcostheta, the work done by gravity is (-150)(20)(cos60) = -1500J. OR more simply, the work by gravity is just weight times vertical distance = (-150)(10) = -1500J.
Similarly, the work done by the person against gravity can be calculated the same way. Note that since this is a constant velocity problem, the net work done by both must be zero, per the work energy theorem.
 

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