Calculating A in SHM from x, v & a

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To calculate the amplitude in simple harmonic motion (SHM) using displacement, velocity, and acceleration, one can utilize conservation of energy principles. The equations of motion for SHM were discussed, revealing that the velocity is zero at maximum amplitude. The user initially struggled with simultaneous equations and the unknowns of phase angle and amplitude but eventually realized that the problem was solvable by expressing energy conservation. A key point of confusion was clarified, distinguishing between the amplitude and the additional distance traveled before the object reverses direction. Ultimately, the user found a solution but noted a discrepancy with the textbook answer, which stemmed from misinterpreting the question's requirements.
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how can you work out the amplitude knowing only displacement, velocity and acceleration?
I have been able to work out angular velocity, frequency and period, but I can't work out amplitude without knowing either the spring constant, the mass or the phase angle.
 
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Welcome to PF,

Why don't you post what you have thus far?

HINT: What is the velocity of the particle when it is at it's amplitude?
 
Hootenanny said:
Welcome to PF,

Thank you, it seems like a nice place :)

Hootenanny said:
Why don't you post what you have thus far?

I have these equations

x=Acos(\omegat+\phi)
v=-A\omegasin(\omegat + \phi)
a=-\omega^{2}cos(\omegat+\phi) =\omegax

I could work out \omega by re arranging the equation for a.

Hootenanny said:
HINT: What is the velocity of the particle when it is at it's amplitude?
It's 0, but I'm still left with two unknown variables, \phi and A, am I not?

edit: why does omega keep showing up as superscript?
 
Have you any initial conditions, such as whether it starts from x=A or x=0?
 
Sorry, I should have typed up the question from the start:
You are watching an object in SHM. When the object is displaced 0.600m to the right of its equilibrium position, it has a velocity of 2.20 m/s to the right and an acceleration of 8.40 m/s^{2} to the left. How much farther from this point will the object move before it stops momentarily and then starts to move back to the left?

I struggled with this for hours and concluded that the question must be wrong, but I went to the homepage of the textbook and downloaded the errata and didn't find anything.
 
It seems to me that you have a system of simultaneous equations.

Which values of \left(\omega t + \phi\right) correspond to the particle being at x=A?
 
Last edited:
when x=A, \left(\omega t + \phi\right)=0

I still can't solve it though, I just end up with division of 0, can you confirm that it really is solvable?
 
Hi mudkip9001,

Try conservation of energy. Equate the energy at the given point to the energy at the amplitude. What do you get?
 
but I don't know neither k nor m
 
  • #10
You'll be able to get rid of them by using what you know about the acceleration.
 
  • #11
What I mean is that although you don't know either k or m, you can find the value of (k/m).
 
  • #12
I just wrote all this, and then figured it out myself just as I finished. But I guess I might as well post t anyway. Thanks for all your help, I'm very relieved now (but I also feel a bit dumb, since I was so sure there was something wrong with the question).

Thanks, I never thought of that. However, I'm still not getting the same answer as the book:

\frac{1}{2}kx^{2} + \frac{1}{2}mv^{2} = \frac{1}{2}kA^{2}

solving for a gives me A=\sqrt{x^{2}+\frac{m}{k}v^{2}}

\frac{-x}{a}=\frac{m}{k}=0.0714

so
A=\sqrt{0.6^{2}+0.0714*2.2^{2}}=0.840m

but the book says 0.240m, where did I go wrong?

where I went wrong was that the question is how much further it would go, not the amplitude.
 
  • #13
What you were missing is squaring the quantity m/k (i.e., A = \sqrt((x^2+v^2)/(x/a)^2)
(Sorry I couldn't write this in pretty-print. I'm new here.)
 
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