Answer: √(k/μ).
- A √(k/μ)
- B √(k(m<sub>1</sub>+m<sub>2</sub>))
- C √(k/m<sub>1</sub> + k/m<sub>2</sub>)
- D √(kμ)
Correct answer: A. √(k/μ)
Explanation: The two-body oscillator reduces to a one-body problem with reduced mass μ. ω = √(k/μ).
In SHM, displacement and velocity are 90° out of phase (v is maximum when x=0, and zero when x is extreme), while acceleration is always exactly opposite in sign to displacement, consistent with a = −ω²x.
Concept context
Simple harmonic motion, spring-mass, pendulum, energy in SHM, and resonance.