Explanations & Calculations
- Refer to the arrangement above & positive measuring direction is positive downward.
- If needed take the spring constant as k.
- Consider the system is released from a distance x down from the normal length level of the spring (then moving upward) and apply Newton's second law on the m kg block.
"\\qquad\\qquad\n\\begin{aligned}\n\\small R-mg&= \\small m(-\\ddot{x})\\\\\n\\small R&= \\small m(g-\\ddot{x}) > 0\\\\\n\\small \\ddot{x}&<g\n\\end{aligned}" : R > 0 while in contact
- Then apply the same to the whole system to analyze the amplitude.
"\\qquad\\qquad\n\\begin{aligned}\n\\small F-3mg&= \\small 3m(-\\ddot{x})\\\\\n\\small- \\ddot{x}&= \\small \\frac{kx-3mg}{3m}<g\\\\\n\\small x&>0\n\\end{aligned}"
- This means that block m stays on 2m in contact, only for the x values measured downward the spring's normal length/ only when the spring is compressed. As soon as the spring relaxes back to it's normal length, m block starts to move under gravity where R = 0.
- And this phenomenon is independent from the amplitude .
Amplitude = "\\begin{aligned}\n\\small \\Big(x-\\frac{3mg}{k}\\Big) \n\\end{aligned}" where "\\begin{aligned}\n\\small \\ddot{x} &= \\small \\frac{-k}{3m}\\Big(x-\\frac{3mg}{k}\\Big)\n\\end{aligned}"
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