Simple Harmonic Motion Solving for the phase and applying it.

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Homework Help Overview

The discussion revolves around a problem involving simple harmonic motion, specifically focusing on a block attached to a spring. The original poster is attempting to determine the amplitude of oscillations, as well as the position and velocity of the block at a specific time.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of equations related to simple harmonic motion, including the position and velocity functions. There is an attempt to derive the phase constant using the ratio of velocity to position, but confusion arises regarding the correct formulas and their application.

Discussion Status

Some participants have pointed out errors in the original poster's approach, particularly regarding the formula for velocity. There is ongoing exploration of the phase constant, with differing results being shared. The conversation indicates that while some progress has been made in calculating the amplitude, there remains uncertainty about the values for position and velocity at time t=0.

Contextual Notes

The original poster is under time constraints due to an impending test, which adds pressure to resolve the problem. There is also a mention of needing to clarify the conditions at t=0, which may not have been adequately addressed in the initial attempts.

Wm_Davies
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Homework Statement


I am having a hard time solving this problem and this is my last chance to solve it before it is due and I have to do this for a test tomorrow.

A simple harmonic oscillator consists of a block of mass 3.90 kg attached to a spring of spring constant 330 N/m. When t = 0.570 s, the position and velocity of the block are x = 0.123 m and v = 3.510 m/s. (a) What is the amplitude of the oscillations? What were the (b) position and (c) velocity of the block at t = 0 s?


Homework Equations



\omega=\sqrt{\frac{k}{m}}
x=x_{m}cos(\omega t + \phi)
v=-\omega x_{m}cos(\omega t + \phi)

The Attempt at a Solution



Okay so I tried to solve for the phase constant by dividing the velocity function by the position function.

This gave me the result of \phi=tan^{-1}(\frac{v}{x \omega})

I plugged in \phi to both the position functions and my answers are wrong. So I am not sure as to what I need to do or why.
 
Last edited:
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Your expression for v should be v=-ωxmsin(ωt+φ)


Also consider what v/x gives and then substitute the conditions to get φ.
 
Yes the formula for velocity was wrong. I divided the two which is how I got \phi is inverse tangen times v divided by the quantity of position times the angular frequency. I must be doing something right because I am able to solve for the amplitude of the function, but I cannot get the position at t=0 and the velocity at t=0.
 
Wm_Davies said:
Yes the formula for velocity was wrong. I divided the two which is how I got \phi is inverse tangen times v divided by the quantity of position times the angular frequency. I must be doing something right because I am able to solve for the amplitude of the function, but I cannot get the position at t=0 and the velocity at t=0.

Could you please post your work on how you found all of your answers?
 
x=x_{m}cos(\omega t + \phi)
v=-\omega x_{m}sin(\omega t + \phi)

So I divided these two functions which gave me the result of...


\omega t + \phi = tan^{-1}(\frac{v}{-x \omega})

Since this is equal to all of the stuff in the position function and the velocity function I put it into the those functions after solving for the amplitude. This cannot lead to a correct answer because the velocity and position in the above mentioned expression are not at time = 0,

P.S. I solved for the amplitude by dividing x at t=.570s by the cos(\omega t + \phi)

which came to... approximately 0.400912 meters
 
What did you get for φ?
 
For \phi I got approximately... 0.240112 radians
 
Recheck it, I get -1.25 radians.
 
Yes I get -1.25897 radians when I solve for \omega t + \phi
 

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