Basic harmonic oscilator problem (but I'm having troble solving it)

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The discussion revolves around solving a harmonic oscillator problem involving two blocks with friction and a spring. The maximum static friction force between the blocks is calculated to be 3.92N, leading to an acceleration of 0.356 m/s² for the system. The angular frequency is determined to be 18.18 rad/s², but confusion arises regarding the phase angle and maximum acceleration conditions. Ultimately, by equating the maximum accelerations of the system and the small block, the correct maximum amplitude is found to be 21.6 cm, resolving the initial misunderstanding. The solution emphasizes the importance of recognizing the relationship between the system's acceleration and the frictional forces.
U.Renko
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Homework Statement


I have small block of mass m=1kg on top of a bigger block mass M=10kg
The friction coefficient between the blocks μ=0.40
No fricton between the big block and the ground.
There is a spring with k=200N/m attached to the bigger block.

The problem asks what is the maximum amplitude A the system can have in an harmonic oscillation without relative motion between the blocks.


Homework Equations



x=A\cos(ωt+\phi)
v=-ωA\sin(ωt+\phi)
a=-ω^2A\cos(ωt+\phi)


The Attempt at a Solution


well, first I noticed that the maximum static force possible between the two blocks will be:
mgμ which gives: (1kg)(9.8m/s^2)(0.40) = 3.92N
so far no problems I guess.

using F=ma, I calculate the acceleration of the system in the case of maximum friction:
a= F/m = (3.92N)/(11kg) which gives a = 0.356m/s^2

using ω^2=k/m=(200N/m)/(11kg) which gives ω^2= 18.18rad/s^2


Now here is where I got stuck
I plug this to a=-ω^2Acos(ωt+\phi) and try solving for A

the thing is:
I don't know the time
I don't know if there is a phase angle involved or not. or how to find out.
 
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When is the acceleration a maximum?
 
Period of a spring is given by T = 2\pi \sqrt{\frac{k}{m}}
Since the problem wants you to solve for the two blocks moving synchronously the phase angle is zero, otherwise they would reach the same points in oscillation at different times (ie one reaches its maximum amplitude as the other is already moving back).
 
well, according to the textbooks the maximum positive acceleration occurs when the body is in its maximum negative position...

then it explains that "combining" the equations for position and acceleration will give a(t)=-ω^2x(t)
which I honestly did not understand why. (I seem to have a problem understanding "combinations" of equations. I'm never sure if they mean adding, dividing or whatever)


Anyway, using this info and the fact explained above by JHamm I find

x= a/-ω^2 = (0.356 m/s^2)/(18.18 rad/s^2) = (0.0196 m)

which is 1.96cm and the answer in the book is 21.6cm ...

so I'm still missing something...
 
You were told that v=-A sin(\omega t+\phi). All you need to know to find the maximum value for that is the maximum and minimum possible values for sine. What are they?
 
The maximum acceleration of the system is a = \frac{\kappa x}{M+m} and the maximum acceleration of the small block is a = \frac{mg\mu}{m} = g\mu. You want these two to equal each other.
 
That's right!

equaling the acceleration of the system with the acceleration of the small block gives
x = 0.2156 m which rounding up gives 21.6 cm


I guess I was fixed in the harmonic oscillator part and didn't quite notice I could do something like this.

Thanks a lot.
 

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