Help on linear momentum and work/energy problems

Click For Summary
SUMMARY

This discussion focuses on solving linear momentum and work/energy problems in physics, specifically addressing six distinct scenarios involving conservation of energy, work done by friction, and the dynamics of pendulums. Key equations mentioned include the Work-Energy Theorem (W = ΔK) and the definition of work (W = Fd). The participants emphasize the importance of understanding energy conservation principles across various contexts, such as gravitational potential energy and kinetic energy. The overarching conclusion is that all problems utilize the same fundamental principle of energy conservation.

PREREQUISITES
  • Understanding of linear momentum and the equation p = mv
  • Familiarity with the Work-Energy Theorem and its application
  • Knowledge of gravitational potential energy (U = mgy)
  • Basic principles of pendulum motion and energy conservation
NEXT STEPS
  • Study the Work-Energy Theorem in detail, focusing on its applications in various scenarios
  • Learn about gravitational potential energy and its calculations in different contexts
  • Explore pendulum dynamics and energy transformations during motion
  • Review examples of friction's impact on work done in mechanical systems
USEFUL FOR

Students and educators in physics, particularly those tackling problems related to linear momentum, work, and energy conservation principles.

SJC25
Messages
6
Reaction score
0
Okay ya'll. I am back with mor eproblems I need help with. I had 18 problems, and I need some guidence on 6 of them.

1) A skier, of mass 60 kg, pushes off the top of a hill with an initial speed of 4.0 m/s. How fast will she be moving after dropping 10 m in elevation?

I am guessing this is a linear momentum problem, but the only equation that fits the info given is p=mv. What do I do with the drop in elevation? I feel like I am going left when I should be going right on this problem.


2) A driver, traveling at 22 m/s, slows down her 1500 kg car to stop for a red light. What work is done by the friction force against the wheels?

Is this a Work-Energy Theorem problem? W (net)= delta K? I know I can find 2 values of K (initial velocity and final)... Am I doing this right?


3) A simple pendulum with a 4.4 kg mass and a length of 75 cm, is released from rest at an angle of 50. (a) To what height does the mass swing on the other side? (b) What is the speed of the mass at the bottom of the swing?

This is the first time I have seen a problem about a pendulum. I can't even find an example in the book. Honestly, I am clueless on this one.


4) A 60 kg woman pushes a 20 kg suitcase on wheels a distance of 10 m by exerting a force of 2.0 N in the direction of motion, starting from rest. (a) How much work does she do? (b) If there were no friction acting on the suitcase, what would its final velocity be at the end of the 10 m distance?

I got part (a)... W=Fd Not sure about part (b)... is it as simple as F=ma, or am I totally wrong again?


5) A workman pushes a 200 kg crate up a frictionless metal ramp pf length 4.00 m into the back of a truck(see figure below) *note= there was no figure below. (a) If the angle made by the ramp with the ground is 25.0 and the workman pushes the block at a very slow, constant speed, how much work does he do? (b) What is the increased gravitational potential energy of the crate?

How do I find work if I don't have a F... which I don't know how to get without an acceleration... I thought about using mgy to find what i need... Am I on the right track?


6) Approximately what running speed would an 80 kg pole-vaulter have to acquire to clear a 5.0 m off the ground? Assume that the pole-vaulter's center of gravity is intially 1.0 m off the ground and that the vaulter clears the bar if his center of gravity just reaches the height of the bar.

Okay, lost on this one too. My book has about 2 paragraphs on center of gravity, and I am just not getting it.
 
Physics news on Phys.org
1) Use an energy approach. Gravity does work on the skier which converts to kinetic energy.
2)Again, use conservation of energy. How much work is needed to put the car to a halt?
3) Once more. Conservation of energy. Gravitational + Kinetic.
4a) Use the definition of work.
b) Use the work energy theorem.
5) Basically the same as 4)
6) Basically the same as 3).

All these questions use the same principle. The total amount of energy is conserved. What is lost in kinetic energy is gained in some other form (usually potential energy).
 
Thanks for the help. I am still having problems with 5 though. How can I find K to do the work energy theorem when I don't have a velocity? Shouldn't I use U=mgy if I am looking for increased gravitational potential energy?
On 4b I have the same problem. How do I use the work energy theorem if I can't find K?
 

Similar threads

Replies
7
Views
2K
Replies
5
Views
2K
Replies
335
Views
18K
  • · Replies 13 ·
Replies
13
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 62 ·
3
Replies
62
Views
14K
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 18 ·
Replies
18
Views
4K
Replies
18
Views
8K
  • · Replies 25 ·
Replies
25
Views
2K