What is the acceleration of a block in simple harmonic oscillation at t=3.0s?

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SUMMARY

The acceleration of a block in simple harmonic oscillation (SHM) at t=3.0 seconds is calculated using the formula a = -ω²A sin(ωt), where ω is the natural frequency and A is the amplitude. For a block with a mass of 0.75 kg attached to a spring with a spring constant of 235 N/m, the natural frequency is determined to be 17.7 rad/s. The correct acceleration at t=3.0 seconds is 13.2 m/s², contrasting with an initial incorrect calculation of -35.2 m/s² due to a misconfiguration of the calculator in degrees instead of radians.

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  • Familiarity with the equations of motion for SHM
  • Knowledge of natural frequency calculation: ω = √(k/m)
  • Ability to differentiate functions for acceleration determination
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fstam2
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Simple Harmonic Oscillation

Hello, I am new here and wish I had found this forum earlier in the semester. Here is the situation:
A block (mass m=0.75 kg) rests on a horizontal surface (frictionless), attached to a horizontal spring (k=235 N/m). At time t=0, the block is located at the equilibrium position (x=0), given a sove that compresses the spring. The block gains a speed of 2.5 m/s instantaneously.
(ii) What is the acceleration of the block at time, t=3.0 s?

The equation I have found that might be correct is:
a= -(kA/m)sin(2(pie)t/T), where t= 3.0s and T=.352 based on
T= 2(pie)sqrt(m/k)
Using this equation I arrived at -35.2 m/s2 (the negative is because of the direction of the acceleration at t= 3.0s). This answer makes sense in that the acceleration has slowed from a max acceleration of 43.8 m/s2.

Any suggestions, advice, criticisms?
Thanks for your help.
Todd
 
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Your equations are true, but I don't see how you got your answer. Like most problems, there's more than one way to do this, but considering the title of your post, consider one of the general forms for SHM of an object:

[itex]x(t) = A\sin(\omega_n t) + B\cos(\omega_n t)[/itex]

where x is the position at time t, ωn is the natural frequency, and A and B are constants determined by the initial conditions. The natural frequency in this problem is:

[itex]\omega_n = \sqrt{\frac{k}{m}}[/itex]

Using the fact that x(0) = 0, we find that B = 0.

The other initial condition is the initial velocity:

[itex]\dot{x}(0) = \omega_n A \cos(\omega_n * (0)) = -2.5\,{\rm \frac{m}{s}}[/itex]

(I have defined compression to be the negative x direction.)

Use this equation (with ωn = 17.7 rad/s) to find A = -0.141 m negative just means it starts moving in compression). You can write the acceleration from the SHM equation as well (by differentiating twice):

[itex]\ddot{x}(t) = -\omega_n^2 A\sin(\omega_n t)[/itex]

Solving for t = 3 s, the acceleration should be 13.2 m/s/s. You should rework the problem to see if I made a mistake, but I think I found your problem: is your calculator in degrees or radians right now? What should it be in? (I wish I noticed that before I blah-blahed the above explanation.)
 
Thanks for your help. I only needed to change my calc. to radians to work out the problem. I never had the manual for the calc., and HP only has the Spanish version to download.
Todd
 

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