Calculating Time for a Mass Hitting a Spring

  • Context: High School 
  • Thread starter Thread starter eggman1965
  • Start date Start date
  • Tags Tags
    Mass Spring Time
Click For Summary

Discussion Overview

The discussion revolves around calculating the time it takes for a mass traveling on a frictionless surface to come to a stop after colliding with a spring, focusing on the physics of simple harmonic motion (SHO) and the relationship between force and time.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes the initial scenario and expresses difficulty in deriving the function for the force versus time graph, noting that while they can calculate distance, they struggle with time.
  • Another participant suggests that knowing the initial velocity and the force allows for the calculation of acceleration, using Hooke's law to relate force and displacement.
  • Some participants mention that the force versus time graph is not linear, with one stating it could be quadratic or exponential, while another later corrects this to sinusoidal.
  • A participant emphasizes that the standard kinematics equations apply only when acceleration is constant, which is not the case here due to the nature of the spring's force.
  • One participant provides a detailed explanation of the equations of motion for SHO, indicating that the time to stop corresponds to one-fourth of a period of oscillation.
  • Another participant calculates the angular frequency and relates it to the time taken to stop, stating that this time is independent of the initial velocity.
  • A later reply acknowledges a previous error regarding the nature of the force versus time graph and confirms the sinusoidal nature of the motion.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the force versus time relationship, with some proposing quadratic or exponential forms while others assert it is sinusoidal. The discussion remains unresolved regarding the best approach to present these concepts in a classroom setting.

Contextual Notes

Participants note that the equations of motion for SHO are necessary to derive the time-related aspects of the problem, and there are unresolved issues regarding the integration of force and its implications for acceleration.

Who May Find This Useful

This discussion may be useful for educators and students interested in the dynamics of simple harmonic motion, particularly in the context of teaching physics concepts related to forces, motion, and energy transfer in spring systems.

eggman1965
Messages
4
Reaction score
0
I posed a question to my gr12 physics class today along these lines:

suppose a mass (m) traveling on a frictionless surface at a speed (v) runs into a spring (constant K). How long (time t) will it take to come to a stop (vf = 0)

I'm quite rusty I suppose since I cannot seem to come up with the function that describes the F vs t graph. Finding the distance is a piece of cake (1/2kx2=1/2mv2) but I'm stuck trying to find the time. Can anyone help?

Thanks
 
Physics news on Phys.org
You have the initial velocity, and you have the force applied to the mass.
Therefore you can find the acceleration of the mass.

F = ma = -kx (by hooke's law)

The sum of the total force applied is equal to:
F = \int_{0}^{x}-kx\hspace{5} dx<br /> <br />

then just divide F by m
find acceleration
then you have the time it takes for Vinitial to change into Vfinal (0)
 
Here's a reminder: Simple harmonic motion.
 
ninevolt said:
You have the initial velocity, and you have the force applied to the mass.
Therefore you can find the acceleration of the mass.

F = ma = -kx (by hooke's law)

The sum of the total force applied is equal to:
F = \int_{0}^{x}-kx\hspace{5} dx<br /> <br />

then just divide F by m
find acceleration
then you have the time it takes for Vinitial to change into Vfinal (0)

AlephZero said:
Here's a reminder: Simple harmonic motion.

This does not give the force vs time relation which is NOT linear. The F vs t graph is either quadratic or exponential and the standard kinematics equations only apply when acceleration is constant (which it is NOT in this case) The S.H.O. is my current focus but I'm still trying to figure out a way to present this to my class in such a way that they can see it.

Thanks Anyway
 
ninevolt said:
You have the initial velocity, and you have the force applied to the mass.
Therefore you can find the acceleration of the mass.

F = ma = -kx (by hooke's law)

The sum of the total force applied is equal to:
F = \int_{0}^{x}-kx\hspace{5} dx<br /> <br />

then just divide F by m
find acceleration
then you have the time it takes for Vinitial to change into Vfinal (0)
The equation is not correct. The integral is not a force but the work of the elastic force.
Dividing it by m will not give acceleration.

In order to find the position, velocity, etc versus time you need to solve the equation of motion.
In this case it is
F/m=a
or -kx/m=d2x/dt2
(F=-kx, a=d2x/dt2)
This is the equation of a SHO and we already know the general solution. So we know that the motion will be a SH motion and can apply the results.

Once the mass connects with the spring, you'll have a SHO.
The initial position corresponds to the zero displacement. It will keep moving until v=0. At this point it will start moving backwards. So the time you are looking for is the time to move between the equilibrium and an extreme, or 1/4 of a period.

Note: edited to correct error. It is 1/4 period and not 1/2 as I wrote originally.
 
Last edited:
eggman1965 said:
This does not give the force vs time relation which is NOT linear. The F vs t graph is either quadratic or exponential
No, it is sinusoidal.

The angular frequency \omega = \sqrt{k/m}

Measuring time from when the mass hits the spring,

x = A \sin \omega t for some constant A.

\dot x = A\omega \cos \omega t

When t = 0 you have \dot x = A \omega = v so A = v/\omega

The time to stop is independent of the velocity and is 1/4 of a complete cycle, so

\omega t = \pi/2 or t = \pi / (2 \omega)

and the standard kinematics equations only apply when acceleration is constant (which it is NOT in this case) The S.H.O. is my current focus but I'm still trying to figure out a way to present this to my class in such a way that they can see it.

Hmm... that could be a tough challenge!
 
AlephZero said:
No, it is sinusoidal.

The angular frequency \omega = \sqrt{k/m}

Measuring time from when the mass hits the spring,

x = A \sin \omega t for some constant A.

\dot x = A\omega \cos \omega t

When t = 0 you have \dot x = A \omega = v so A = v/\omega

The time to stop is independent of the velocity and is 1/4 of a complete cycle, so

\omega t = \pi/2 or t = \pi / (2 \omega)



Hmm... that could be a tough challenge!

Thank you! This is what I was looking for, and yes my rust is showing as it is of course a sine function not a quadratic/exponential as I erroneously stated earlier.

Sincerely

eggman1965
 

Similar threads

  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 17 ·
Replies
17
Views
3K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 13 ·
Replies
13
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 20 ·
Replies
20
Views
4K
  • · Replies 8 ·
Replies
8
Views
1K
  • · Replies 2 ·
Replies
2
Views
2K