Solve Rod Slider Energy Problem: Find Velocities of Collar B

AI Thread Summary
The discussion revolves around solving the energy problem of Collar B, which is influenced by a spring and set in motion with given parameters. The conservation of energy principle is emphasized, with attempts to calculate the radial and transverse components of velocity when the collar's position changes. One participant struggles to find the correct radial velocity and seeks guidance on determining the tangential velocity without using angular momentum, as it hasn't been covered in class. Suggestions include using the work-energy principle and focusing on the total mechanical energy, which remains constant due to conservative forces. The conversation highlights the importance of integrating kinetic and potential energy concepts to solve the problem effectively.
stinlin
Messages
72
Reaction score
1

Homework Statement


Collar B has a mass of 4 kg and is attached to a spring of constant 1500 N/m and of undeformed length 0.4 m. The system is set in motion with r = 0.2 m, v_theta = 6 m/s, and v_r = 0. Neglecting the mass of the rod and the effect of friction, determine the radial and transverse components of the velocity of the collar when r = 0.5 m.


2. Relevant theories

Conservation of energy - kinetic and potential energy

The Attempt at a Solution



I used conservation of energy :

V_spring_initial = V_spring_final + T_slider_final

x_initial_spring = abs(0.2-0.4)
x_final_spring = abs(0.5-0.4)


I solved for v_r and got 3.35 m/s, which is NOT the right answer.

If I figure out how to solve for v_r, I'm still in the situation where I don't really know how to solve for v_theta. I'm thinking I can determine the force due to the spring and set that equal to m*a_normal, solve for v_theta there (because v^2 = (v_tangential)^2 = (v_theta)^2).

Can I get some help? Thanks a bunch!
 

Attachments

  • 1393.GIF
    1393.GIF
    6.5 KB · Views: 527
Physics news on Phys.org
Use conservation of angular momentum to find the velocity in the tangential direction as a function of the radius.

Use a net force equation to find the velocity in the radial direction as a function of the radius. (You can consider it as an "inertial" frame with a fictional force, if you want.)
 
We haven't done angular momentum in class yet. While I do know it, he wants us to try and stick to the concepts we know.
 
Is there any more thoughts on this one or no??
 
If one looks at just the SHM motion of the slider its energy stays constant throughout the motion:

\frac{1}{2}Ax^2

which enables one to calculate the radial velocity at any position.

Looking at the bigger picture the total mechanical energy (which will stay
constant since the slider is subject to a conservative force) of the slider should also include its rotational kinetic energy:

\frac{1}{2}I\omega ^2

, where its rotational velocity is determined by the tangential velocity.
 
Last edited:
But the concept of moment of inertia hasn't been formally introduced in our class yet, so we can't really use that equation.
 
How did you get the answer for Vr? What principle did you use? I was going to suggest you use the work-energy principle.
 
stinlin said:
But the concept of moment of inertia hasn't been formally introduced in our class yet, so we can't really use that equation.

Ok. You can then still use the fact that T + V will stay constant. The speed that you get will be the real speed of the slider, that is the tangential and radial speed combined or just v.
 
Back
Top