Easy Conservation of Energy Problem

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SUMMARY

The discussion centers on a physics problem involving a skier of mass 55.0 kg sliding down a slope of length 11.7 m, with an initial speed of 0.657 m/s and a final speed of 7.19 m/s. The kinetic friction acting on the skier is 41.5 N. Participants analyze the application of the law of conservation of energy, specifically using the equations for kinetic energy (Ek = 1/2*m*v^2), gravitational potential energy (Eg = mgh), and work done by friction (Ethermal = W = Fk*cosθ*Δd). The challenge lies in determining the angle θ of the slope, with discussions highlighting the role of friction and the cosine of the angle in energy calculations.

PREREQUISITES
  • Understanding of kinetic energy and gravitational potential energy equations
  • Familiarity with the concept of work and friction in physics
  • Basic knowledge of trigonometry, particularly sine and cosine functions
  • Ability to apply the law of conservation of energy in problem-solving
NEXT STEPS
  • Study the derivation and application of the law of conservation of energy in various contexts
  • Learn about the effects of friction on motion, including the role of angles in energy loss
  • Explore circular motion problems and the impact of friction at different angles
  • Practice solving energy conservation problems involving inclined planes and friction
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and energy conservation, as well as educators looking for examples of applying theoretical concepts to practical problems.

BioBabe91
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Homework Statement


A skier of mass 55.0 kg slides down a slope 11.7 m long, inclined at an angle θ to the horizontal. The magnitude of kinetic friction is 41.5 N. The skier's initial speed is 65.7 cm/s (0.657 m/s) and the speed at the bottom of the slope is 7.19 m/s. Determine the angle θ from the law of conservation of energy. Air resistance does not matter.


Homework Equations


Ek = 1/2*m*v^2
Eg = mgh
Ethermal = W = Fk*cosθ*Δd

The Attempt at a Solution


Eth= Fk*cosθ*Δd
Substituted in the values, then used conserv. of energy:
mgh + 1/2*mv^2 = 1/2*mv^2 + Eth
where h = 11.7/sinθ.
But I got stuck solving for the angle. Where did I go wrong?
 
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I think the work from the kinetic friction is taken over the length of the incline because the cosφ relative to the motion of the skier is 0, along the plane of the slope, not the angle θ of the incline.

Otherwise, I think you have the right idea.
 
That's true. But in what cases would cosφ not be equal to 0, for future questions like this?

Thanks.
 
BioBabe91 said:
That's true. But in what cases would cosφ not be equal to 0, for future questions like this?

Thanks.

For friction I'd guess that the angle φ is usually always 0, if it acts against the direction of motion. Now on circular motion problems, friction that would be say keeping a car from sliding down an incline would contribute no energy loss because there the friction would be at 90°

Work = F ⋅ D

(which is the dot product if you are familiar with vectors)
 

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