Work Done: Which Initial Velocity is Most Effective?

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SUMMARY

The discussion centers on the concept of work done in physics, specifically in relation to initial velocity and its effect on work performed on a block. The work-energy theorem is highlighted, stating that the work done (W) is equal to the change in kinetic energy (ΔK), expressed as W = K_f - K_i. The participants clarify that the direction of initial velocity does not affect the total work done, as the distance traveled remains constant regardless of direction. The consensus is that the only work done in the first scenario is by the man rubbing his hands together due to friction.

PREREQUISITES
  • Understanding of the work-energy theorem
  • Familiarity with the equation W = Fd cos(θ)
  • Basic knowledge of kinetic energy equations
  • Concept of forces acting on objects in motion
NEXT STEPS
  • Study the work-energy theorem in detail
  • Learn about the relationship between force, displacement, and work
  • Explore the implications of initial velocity on kinetic energy
  • Investigate examples of work done in various physical scenarios
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Students studying physics, educators teaching mechanics, and anyone interested in understanding the principles of work and energy in motion.

vivekfan
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Homework Statement



1) In which of the following situations is work done?

A man rubs his hands together and they get warm or the moon orbits the earth?

2) A man pulls a 100 kg block across a frictionless floor using a rope. The rope makes an angle of 60 degrees with the horizontal and the man pulls with a force of 50 N. The block moves across the surface 20 m.

Assume the force acts for a time t. Assume the block has initial velocity v. Initial velocity in which direction would result in the greatest amount of work done on the block?

a) Initial velocity to the left
b)Initial velocity to the rightt
c)Initial velocity in either direction would result in the same amount of work done because distance traveled would be the same.
d)Initial velocity in either direction would result in the same amount of work done because the time t is constant.
e)none of the above.

Homework Equations



W=Fdcos(theta)

The Attempt at a Solution



For the first question, I'm pretty sure the only work done is by the man rubbing his hands together, because it's work done by friction. The moon orbiting the Earth is a circular path, so the displacement would be tangent (or perpendicular) to the inward force, right? I'm not sure if my reasoning is correct.

For the second question, I'm pretty confused.

I don't understand what velocity has to do with work, given the equation, and I'm not sure what's really happening in the question with regard to forces. Please help. Thanks!
 
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vivekfan said:

The Attempt at a Solution


For the first question, I'm pretty sure the only work done is by the man rubbing his hands together, because it's work done by friction. The moon orbiting the Earth is a circular path, so the displacement would be tangent (or perpendicular) to the inward force, right? I'm not sure if my reasoning is correct.

Yes, that's right.

For the second question, I'm pretty confused.

I don't understand what velocity has to do with work, given the equation, and I'm not sure what's really happening in the question with regard to forces.

Work and velocity are related via the work-energy theorem. The work W done on the box is equal to the change in kinetic energy \Delta K of the box. So...


W=\Delta K

W=K_f-K_i

W=\frac{1}{2}mv_f^2-\frac{1}{2}mv_i^2
 
Tom Mattson said:
Yes, that's right.



Work and velocity are related via the work-energy theorem. The work W done on the box is equal to the change in kinetic energy \Delta K of the box. So...


W=\Delta K

W=K_f-K_i

W=\frac{1}{2}mv_f^2-\frac{1}{2}mv_i^2

But what does this have to do with the direction of initial velocity?
 

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