Work, Kinetic Energy, Spring, Friction Problem

Click For Summary
SUMMARY

The discussion focuses on a physics problem involving a block sliding on a track with varying conditions, including gravitational force, normal force, and friction. Key calculations include the work done by gravitational force (W = mgh), the work done by friction in the rough region (W_friction = -0.49 J), and the speed of the block before reaching the spring (2.73 m/s). The spring's work and compression distance are also analyzed, emphasizing the conservation of energy and the work-energy theorem.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with the work-energy theorem
  • Knowledge of kinetic and potential energy equations
  • Basic principles of friction and spring mechanics
NEXT STEPS
  • Study the work-energy theorem in detail
  • Learn about the equations for spring potential energy (W = 1/2 k x^2)
  • Explore the effects of friction on motion in physics
  • Investigate conservation of energy in mechanical systems
USEFUL FOR

Students studying physics, educators teaching mechanics, and anyone interested in understanding energy conservation and work in physical systems.

Tristin_noel
Messages
1
Reaction score
0
A block slides from rest, along a track with an elevated left end, a flat central part, into a relaxed spring, as shown in the figure. The curved portion of the track is frictionless, as well as the first portion of the flat part of L = 10 cm. The coefficient of kinetic friction between the block and the only rough part, D = 10 cm, is given by uk = 0.20. Let the initial height of the block be h = 40cm, its mass be m = 2.5 kg, and the spring constant k = 320 N/m. (Picture should be posted below.)

1. While the block slides through the flat central part of length L find:

a) The work done on the block by the gravitational force. = would you use W=mgh ?
b) The work done on the block by the normal force. = 0 bc the normal force is perpendicular to the displacement.
c) The work done on the block by the frictional force. = 0 bc no frictional force present
d) The speed of the block right before it reaches the beginning of the rough central part of length D. =2.8m/s used the eqautopn PE=KE , mgh=1/2m(vf^2-vi^2)

2) The block has now made it to the rough region of length D and will eventually slide head on into the spring at the end of the path. Over this region of length D, calculate:

e) The work done on the block by the gravitational force. = 0 bc perpendicular
f) The work done on the block by the normal force. = 0 bc perpendicular
g) The work done on the block by the frictional force. =-0.49J bc Wfriction=uk(mg)d
h) The speed of the block just as it reaches the spring. =2.73m/s using Vf^2-Vi^2=2(-ukg)d

3) Assuming the block compresses the spring by x, find:

i) The work done by the spring force. would you use W=1/2mVf^2 ?
j) The compression distance, x, of the spring. would you use W=kx and just solve for x?

https://s.yimg.com/hd/answers/i/6ae6d9b8385d4d3eb364c25c31aeb7d5_A.png?a=answers&mr=0&x=1425534324&s=478f148cd3470b7f93d03b19b2553c0b
 
Last edited by a moderator:
Physics news on Phys.org
The point of the exercise is to test/improve your understanding of conservation of energy and work.
Your questions are about what equations to use - you should use your understanding, which seems OK, to figure out the equations.
How would you go about answering your own questions? i.e. for (a) you want to know if the work due to falling a distance h under gravity is given by mgh.
How could you check? Perhaps by using the definition of work in terms of forces or in terms of the work-energy theorem?
Same for the work done by the spring.
 

Similar threads

  • · Replies 18 ·
Replies
18
Views
1K
  • · Replies 58 ·
2
Replies
58
Views
3K
Replies
17
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 29 ·
Replies
29
Views
1K
  • · Replies 12 ·
Replies
12
Views
3K
Replies
29
Views
3K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 37 ·
2
Replies
37
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K