Question about two falling masses connected with a spring

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SUMMARY

The discussion revolves around solving a differential equation related to two falling masses connected by a spring. The equation is given as m(d²y/dt²) + 2ky = mg, leading to the complete solution z(t) = (mg/2k) + c₁cos(√(2k/m)t) + c₂sin(√(2k/m)t). The user expresses confusion regarding the mathematical coherence of the solution provided in a referenced thread and proposes an alternative equation m(d²z/dt²) + 2kz = 0, which accurately reflects the system's dynamics. The user ultimately clarifies their understanding of the relationship between accelerations relative to the ground and the center of mass.

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Mohammad
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Hi, this is my first post :)

I have a question in reference to the same problem in: https://www.physicsforums.com/showthread.php?t=67697&highlight=Falling+Mass

I am having trouble comprehending the 3rd part.

I understand that the differential equation to solve is:
[tex]m\frac{d^2y}{dt} + 2ky = mg[/tex]

Solving this equation yields the following complete solution:
[tex]z(t) = \frac{mg}{2k} + c_1cos(\sqrt{2k/m}t) + c_2sin(\sqrt{2k/m}t)[/tex]

I am stuck at this point. The solution the author posted in the above-mentioned topic doesn't seem coherent to me from a mathematical point of view. Any guidance would be appretiated.
 
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Mohammad said:
Hi, this is my first post :)

I have a question in reference to the same problem in: https://www.physicsforums.com/showthread.php?t=67697&highlight=Falling+Mass

I am having trouble comprehending the 3rd part.

I understand that the differential equation to solve is:
[tex]m\frac{d^2y}{dt} + 2ky = mg[/tex]
It appears to me that the differential equation should be:
[tex]m\frac{d^2z}{dt} + 2kz = 0[/tex]

Where z is the distance of the bottom mass from the center of mass of the system.

The acceleration of the bottom mass is (mg-kx)/m and the acceleration of the entire system is g. So the relative acceleration is (mg-kx)/m - g
=-kx/m = -2kz/m (since z=1/2 the total extension x). a=-2kz/m leads to the diff. eq above.

Complete solution is (as you posted but without one term):
[tex]z(t)=c_1cos(\sqrt{2k/m}t) + c_2sin(\sqrt{2k/m}t)[/tex]

Solving this with z(0)=mg/2k and z'(0)=0 gives the particular solution:

[tex]z(t)=(mg/2k) cos(\sqrt{2k/m}t)[/tex]
 
Thank you for your reply. I can understand what is going on now. I was basically mixing up the acceleration relative to the ground with the acceleration relative to the center of mass.
 

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