Solving a Physics Homework Problem: Work, Distance, & Normal Force

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SUMMARY

This discussion focuses on solving a physics homework problem involving a block propelled by a compressed spring along a frictionless path, transitioning through a frictional area and a loop-the-loop. Key calculations include the work done by friction using the equation W_f = \mu_k m g L, the distance the spring was compressed derived from conservation of energy, and the normal force at the top of the loop calculated using centripetal force principles. The correct approach for the normal force involves adjusting kinetic energy calculations to account for energy transitions between locations.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with conservation of energy principles
  • Knowledge of Hooke's law and spring mechanics
  • Basic concepts of circular motion and centripetal force
NEXT STEPS
  • Study the application of conservation of energy in mechanical systems
  • Learn about the dynamics of circular motion and centripetal acceleration
  • Explore the implications of friction in energy loss during motion
  • Review Hooke's law and its applications in real-world scenarios
USEFUL FOR

Students studying physics, particularly those tackling mechanics problems involving energy, friction, and circular motion. This discussion is beneficial for anyone preparing for exams or needing clarification on these concepts.

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Homework Statement


A compressed spring is released pushing a block at rest along a level, frictionless path. This is Location 1. The block then passes over a small area of friction which ends and becomes frictionless again. This is Location 2. The block then enters a loop-the-loop in the shape of a circle under no apparent acceleration. The top of this loop is Location 3. The block then completes the loop, and continues to travel on a level, frictionless path towards a 90 degree arc which launches the block vertical to a point, Location 4.

Given is the mass of the block(m), coefficient of kinetic friction(\mu_k), length of the area with friction(L), the spring constant(k), diameter of the circular(D) loop-the-loop, height of the point Location 4(y).

a) Find the work done by friction.
b) Find the distance the spring was compressed.
c) Find the normal force at the top of the loop.


Homework Equations


f_k = \mu_k m g
W = \vec{F} \Delta \vec{r}
K_i + U_i = K_f + U_f
K = \frac{1}{2} m v^2
U = m g y
U_s = \frac{1}{2} k x^2 - Hooke's law
\sum F_c = m a_c = \frac{m v^2}{r}


The Attempt at a Solution



a) My current solution simply involves combining the friction force equation and putting that into the equation for work.
W_f = \mu_k m g L

This is the energy lost from Location 1 to Location 2.

b) Using conservation of energy, find the energy required to go from Location 2 to 4.
K_2 + U_2 = K_4 + U_4
K_2 = U_4 = m g y

Energy at Location 0 is equal to work done by friction between Location 1 and 2 and the potential energy at height y.
K_1 = K_2 + W_f
U_0 = K_1
x = \sqrt{\frac{2 U_0}{k}}

c) Converting kinetic energy to linear velocity, find the speed the block enters the loop.
r = \frac{D}{2}
K_2 = \frac{m v^2}{2}
v_2 = \sqrt{\frac{2 K_2}{m}}
F_{c,top] = \frac{m v^2}{r} = m g + F_{N,top}
F_{N,top} = \frac{m v^2}{r} - m g
 
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I think I needed to change my part C calculation as K_2 = K_3 +U_3. Then solve for K_3 and then convert kinetic into velocity. So F_{N,top} = \frac{2 K_3}{r} - m g. I think that is the correct way to calculate it.
 

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