Question about two falling masses connected with a spring

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The discussion centers on solving a differential equation related to two falling masses connected by a spring. The equation m(d²y/dt²) + 2ky = mg is identified, with the user expressing confusion over the solution provided in another thread. They propose an alternative equation m(d²z/dt²) + 2kz = 0, focusing on the distance of the bottom mass from the center of mass. The user clarifies their misunderstanding regarding the relative accelerations, which helped them grasp the solution better. Overall, the conversation highlights the complexities of analyzing motion in a system with connected masses and springs.
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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:
m\frac{d^2y}{dt} + 2ky = mg

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

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:
m\frac{d^2y}{dt} + 2ky = mg
It appears to me that the differential equation should be:
m\frac{d^2z}{dt} + 2kz = 0

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):
z(t)=c_1cos(\sqrt{2k/m}t) + c_2sin(\sqrt{2k/m}t)

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

z(t)=(mg/2k) cos(\sqrt{2k/m}t)
 
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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