Force & Oscillations of 2.12 kg Mass on Frictionless Track

Click For Summary

Homework Help Overview

The problem involves a 2.12 kg mass attached to a spring on a frictionless track, undergoing simple harmonic motion after being displaced from its equilibrium position. The discussion focuses on determining the force acting on the mass after a specific time and the number of oscillations within that time frame.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore various methods to link simple harmonic motion with kinematics, including the use of Hooke's Law and conservation of energy.
  • Some participants question the appropriateness of using total distance versus displacement from equilibrium in their calculations.
  • There is discussion about the correct application of equations for position and force in the context of oscillation.

Discussion Status

Participants are actively engaging with the problem, offering different perspectives and methods. Some have provided guidance on using trigonometric functions to express position in simple harmonic motion, while others emphasize the importance of understanding displacement relative to equilibrium. The conversation reflects a productive exploration of concepts without reaching a definitive consensus.

Contextual Notes

Participants note the need to clarify the distinction between total distance traveled and displacement from the equilibrium position, as well as the implications of the phase constant in the equations of motion.

DDS
Messages
171
Reaction score
0
A 2.12 kg mass on a frictionless horizontal track is attached to the end of a horizontal spring whose force constant is 4.83 N/m. The mass is displaced 3.12 m to the right from its equilibrium position and then released, which initiates simple harmonic motion. What is the force (including direction, choose the right to be positive) acting on the mass 3.46 s after it is released?
B) How many times does the mass oscillate in 3.46 s?

The above is my problem. I am having a hard time linking the SHM aspects with the kinematics aspects.

I have calculated my w, found my period and frequency but i don't know where to take it from there. Any suggestions?
 
Physics news on Phys.org
I have also taken another approach to solving this question, i am thinking of using conservation of energy and solving for v and then plugging that into the impulse forumal but i am not sure if that would be solving the problem incorrectly since the system is obeying SHM
 
The first half can be solved via a direct application of Hooke's Law.
 
I don't think it can because the block is displaced to the a particular side. Its not displaced in a plane.

Plus i tried to solve it that way and the answer is wrong.

Anyone elese?
 
DDS said:
I don't think it can because the block is displaced to the a particular side. Its not displaced in a plane.
This doesn't make sense. It is displaced along the axis of the spring, is there something I'm missing?

Plus i tried to solve it that way and the answer is wrong.

Anyone elese?

You need to find the position at t=3.46sec. It is asking for the force at this time.
 
whozum, I am really sorry i misread my own question. I was confusing it with another one. Really sorry
 
Thats fine, do you need any more help?
 
Now that i know what its asking,

i found the velocity of the block and the total distance its traveled in that time span but when i plug back into hookes law i get a fairly large answer. Which results in it being wrong. How would i best go about finding its position at the given time interval?
 
Hooke's Law requires the displacement from the equilibrium position. You probably are entering the total distance covered by the oscillating block, which is not what you need, you need the distance between the position at t=3.46s and the equilibrium position (t=0 for this case).
 
  • #10
Let me show you what I've done so far:
.5kx^2=.5mv^2
v=4.7

d=v*t
=16.262 this becomes my displacement from eqm.

subbing into hookes law i get

F=56.2 N
 
  • #11
DDS said:
Let me show you what I've done so far:
.5kx^2=.5mv^2
v=4.7

The equation you cited above gives the kinetic energy of an object due to its PE from the spring's displacement. It is not suitable for this specific problem. Also note that in the spring, the velocity for simple harmonic motion is NOT constant. Surely you have expressed SHM problems in terms of sine and cosine functions, this application is what you need to use for this problem.

d=v*t
=16.262 this becomes my displacement from eqm.

subbing into hookes law i get

F=56.2 N

Again, that would be the TOTAL displacement that the mass has experienced in the 3.46 seconds. This is not what you are looking for, you want to find the distance that the block is form its original starting position. Since it is in SHM it is oscillating about the equilibrium point, it just keeps going back and forth in the same location, so it is easy to see that AT MOST this value will be that of the wave's amplitude.

If it had traveled 16.262m total, it would not be 16.262 meters away, it would have made several 'laps' around the origin and returned to a previous position within the lap (kind of like a swimmer swimming 300m in a 50m pool, he is not 300m away from where he started, instead he is exactly where he started.)
 
  • #12
Yes i see what you are saying:

would i have to manipulate

x(t)=Acos(wt +pi) in order to find my amplitude.

I have a feeling that it takes 1/4 of oscialtiong to reach its max distance or let's say amplitude
 
  • #13
You could definitely do it that way, however the pi in the equation should be a theta, and the trig function should (doesnt have to be for correct values of theta) be a sin function as opposed to a cosine.

If you know some calculus, you could easily find the force from the above equation knowing that acceleration is the second derivative of position..
 
Last edited:
  • #14
DDS said:
Yes i see what you are saying:

would i have to manipulate

x(t)=Acos(wt +pi) in order to find my amplitude.

I have a feeling that it takes 1/4 of oscialtiong to reach its max distance or let's say amplitude

[tex]x(t) = A cos(\omega t + \phi)[/tex]

at t = 0, x = A. Use this fact to determine the phase constant. Then proceed with Hooke's law as you planned.
 
  • #15
There is an easier way.

Use the equation for acceleration as a function of time. Then Newton's 2nd Law.
 
  • #16
Chi Meson said:
There is an easier way.

Use the equation for acceleration as a function of time. Then Newton's 2nd Law.

That is another way, but why is that easier?

In the first x = ..., F = kx,

In the second a = ..., F = ma.
 
  • #17
Point taken. It is equivalent to your solution. Both are much easier than the direction this thread was going.
 
  • #18
Thanks everyone i got the answer
 
  • #19
Chi Meson said:
Point taken. It is equivalent to your solution. Both are much easier than the direction this thread was going.

The thread was going to this same conclusion, if you read my last post.
 

Similar threads

Replies
17
Views
3K
Replies
1
Views
2K
Replies
27
Views
3K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
2
Views
2K
Replies
13
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
8
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K