Simple Harmonic Motion of a bolt of mass

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Homework Help Overview

The discussion revolves around simple harmonic motion (SHM) involving a bolt and a glider on a frictionless air track. The original poster presents a problem regarding the displacement of a bolt in SHM, providing specific parameters such as mass, amplitude, and period. Another participant introduces a related problem concerning a glider attached to a spring, questioning the interpretation of acceleration data from a graph.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to calculate the displacement of a bolt using the cosine function for SHM, while others discuss the implications of using acceleration data from a graph to determine maximum displacement and the relationship between force, mass, and amplitude.

Discussion Status

Participants are actively engaging with the problems, offering insights and methods for approaching the calculations. Some have provided guidance on using force equations and interpreting graphs, while others are exploring the implications of their findings without reaching a definitive conclusion.

Contextual Notes

Participants are navigating the complexities of SHM and the integration of acceleration data, with some expressing uncertainty about constants of integration and initial conditions. There is mention of homework constraints and the need to derive relationships from provided data.

QuarkCharmer
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Homework Statement


A bolt of mass 2.10×10^-2 kg moves with SHM that has an amplitude of 0.245 m and a period of 1.495 s. The displacement of the bolt is + 0.245 m when t=0.

A.) Find the displacement of the bolt at time t=0.500s


Homework Equations




The Attempt at a Solution



Part A.)
ω= \frac{2π}{1.495}
ω= 4.20

Since the function starts at +0.245 I modeled the motion by this:
x(t) = Acos(ωt + \phi)
x(t) = 0.245cos(4.20t)

I then evaluated x(t) at t = .5 and I got that:
x(.5) = -.123

Make sense?

(There are more parts to this problem, but I wanted to make sure I remember graphing of trig functions correctly.)
 
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QuarkCharmer said:
Make sense?

Perfectly! :smile:
 
I like Serena said:
Perfectly! :smile:

Great! (Also, Happy Halloween ILS)

Now I am stuck with this one:

On a frictionless, horizontal air track, a glider oscillates at the end of an ideal spring of force constant 4.00 N/cm. The graph in the figure shows the acceleration of the glider as a function of time.

k = 400 N/m

I found the mass of the glider to be 0.405 kg.

2ai3rde.jpg


Find the maximum displacement of the glider from the equilibrium point.
I don't understand how this is possible, considering it's a graph of acceleration vs. time. I lose information in the form of the constant of integration? Can you point me in the right direction on this part?
 
Alas, no Halloween where I live!

How did you find the mass of the glider?
Anyway, with it you can use F=kx=ma to find the amplitude.

Alternatively, SHM has x=A cos wt (starting from some irrelevant time in this case).
Take the derivative twice and you get the equation for acceleration a.
You should be able to use the information in the graph to figure out A.
 
I like Serena said:
Alas, no Halloween where I live!

How did you find the mass of the glider?
Anyway, with it you can use F=kx=ma to find the amplitude.

Alternatively, SHM has x=A cos wt (starting from some irrelevant time in this case).
Take the derivative twice and you get the equation for acceleration a.
You should be able to use the information in the graph to figure out A.

I can read the amplitude (of acceleration) from the graph, and integrate the function into:
\upsilon(t)=\frac{1.2}{\pi}cos(10\pi t) + C
But I can't manage to get an initial condition (or whatever you call it in this case) where I can solve for the constant and continue to integrate.

Edit: Or can I say that since velocity is zero when acceleration is at it's minimum, (and acceleration hits a min at t=.25), then v(.25) = 0, and thus C = 0?I'll see what I can put together with F=ma.

F = -kx = ma
-kx = ma
-(400)x = (0.405)(12)
x_{amplitude} = 0.01215 m

0.01215 m \frac{100cm}{1m} = 1.215 cm
1.22 cm is the Amplitude of displacement vs time?

If that is correct, then:
"Find the maximum force the spring exerts on the glider. "
Would simply be:
F = ma
F = (0.405)(12) (assuming force is max when accel is max)
F = 4.86 N

That just seems like a low number?
 
Last edited:
But it's correct!

Thank you!
Edit: Oh and I found the glider mass by reading the period off the acceleration/time graph and then applying:
T = 2 \pi \sqrt{\frac{m}{k}}
 
Last edited:
QuarkCharmer said:
I can read the amplitude (of acceleration) from the graph, and integrate the function into:
\upsilon(t)=\frac{1.2}{\pi}cos(10\pi t) + C
But I can't manage to get an initial condition (or whatever you call it in this case) where I can solve for the constant and continue to integrate.

Edit: Or can I say that since velocity is zero when acceleration is at it's minimum, (and acceleration hits a min at t=.25), then v(.25) = 0, and thus C = 0?

Yep! :wink:
 
QuarkCharmer said:
But it's correct!

Thank you!



Edit: Oh and I found the glider mass by reading the period off the acceleration/time graph and then applying:
T = 2 \pi \sqrt{\frac{m}{k}}


Aha! :smile:
 

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