Oscillations and SHM: Real-World Scenarios (8)

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Question

A 200 g block hangs from a spring and stretches it by 5 cm at rest. The block is then pulled down 3 cm and released. Find the period of oscillation and the maximum speed. Take g=10 m/s2g = 10\text{ m/s}^2.

Solution — Step by Step

At equilibrium, the spring force balances gravity:

kx0=mg    k=mgx0=0.2×100.05=40 N/mk x_0 = mg \implies k = \frac{mg}{x_0} = \frac{0.2 \times 10}{0.05} = 40\text{ N/m}

T=2πmk=2π0.240=2π0.0050.444 sT = 2\pi\sqrt{\frac{m}{k}} = 2\pi\sqrt{\frac{0.2}{40}} = 2\pi\sqrt{0.005} \approx 0.444\text{ s}

Amplitude A=0.03 mA = 0.03\text{ m}. Angular frequency ω=k/m=20014.14 rad/s\omega = \sqrt{k/m} = \sqrt{200} \approx 14.14\text{ rad/s}.

vmax=ωA=14.14×0.030.424 m/sv_{max} = \omega A = 14.14 \times 0.03 \approx 0.424\text{ m/s}

Final answer: T0.44 sT \approx 0.44\text{ s}, vmax0.42 m/sv_{max} \approx 0.42\text{ m/s}

Why This Works

The neat trick of the vertical spring: gravity just shifts the equilibrium position. Once we measure the oscillation from this new equilibrium, the SHM equations are identical to a horizontal spring. That is why T=2πm/kT = 2\pi\sqrt{m/k} has no gg in it, even though gravity is acting.

The static stretch x0=mg/kx_0 = mg/k is a free measurement of kk — no need for force gauges or any other setup.

Alternative Method

We can find vmaxv_{max} via energy conservation: at the extreme, all energy is potential (12kA2\frac{1}{2}kA^2); at equilibrium, all is kinetic (12mvmax2\frac{1}{2}mv_{max}^2).

vmax=Ak/mv_{max} = A\sqrt{k/m}

Same answer, sometimes faster if ω\omega is messy.

Common Mistake

Students plug A=0.05A = 0.05 m (the static stretch) instead of A=0.03A = 0.03 m (the pull-down distance). The amplitude is whatever the block is displaced from the new equilibrium, not from the natural length of the spring.

This setup with slightly different numbers appeared in NEET 2022. The trick is always the same: use the static stretch to find kk, then forget about gravity entirely.

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