1. A simple pendulum has length 1 m. Taking g = π² m/s², its time period is:
- 3 s
- 4 s
- 1 s
- 2 s
Show answer and explanation
Answer: (D) 2 s
For a simple pendulum T = 2π√(L/g). With g = π², T = 2π√(1/π²) = 2√1 = 2 s.
56 questions on this topic of Oscillations and Waves (NEET 2027 syllabus). Here are 12; tap one to see its answer and explanation.
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Answer: (D) 2 s
For a simple pendulum T = 2π√(L/g). With g = π², T = 2π√(1/π²) = 2√1 = 2 s.
Answer: (D) 8
The ratio of their time periods is T₁ / T₂ = √(L₁ / L₂) = √(64 / 49) = 8 / 7. Let n₁ and n₂ be the number of oscillations completed by the longer and shorter pendulums respectively when they come into the same phase again. Then n₁ T₁ = n₂ T₂, which gives n₁ / n₂ = T₂ / T₁ = 7 / 8. Thus, the shorter pendulum completes n₂ = 8 oscillations.
Answer: (C) (3/2) π √(L/g)
For one half of the oscillation (say, to the left), the pendulum swings freely with length L, taking time t₁ = (1/2) × 2π√(L/g) = π√(L/g). For the other half (to the right), the string bends around the nail, so effective length is L - 3L/4 = L/4, taking time t₂ = (1/2) × 2π√(L/(4g)) = (π/2)√(L/g). Total period T = t₁ + t₂ = π√(L/g) + (π/2)√(L/g) = (3/2)π√(L/g).
Answer: (C) Infinite
Inside an orbiting spacecraft, all objects are in a state of free fall, so the effective acceleration due to gravity is g_eff = 0. Therefore, the time period T = 2π√(L/g_eff) becomes infinite.
Answer: (D) 20%
The time period is related to length by T ∝ √L. If the new length is L' = L - 0.36L = 0.64L, then the new time period is T' = √(0.64) T = 0.8 T. The percentage decrease in time period is ((T - T') / T) × 100% = (1 - 0.8) × 100% = 20%.
Answer: (A) 12 hours
At height h = R, the acceleration due to gravity is g' = g(R/(R+R))² = g/4. The time period becomes T' = 2π√(L/g') = 2T. Since the pendulum takes twice as long per oscillation, the clock runs at half the normal rate, showing only 12 hours in a 24-hour day and losing 12 hours.
Answer: (B) 6
The time periods are T₁ = 2π√(1.44/g) ∝ 1.2 and T₂ = 2π√(1.00/g) ∝ 1.0. Thus, T₁/T₂ = 1.2/1.0 = 6/5. For them to be in phase again, n₂ T₂ = n₁ T₁, which gives n₂/n₁ = T₁/T₂ = 6/5. Hence, the shorter pendulum completes 6 oscillations when the longer completes 5.
Answer: (B) 1.4 s
For a simple pendulum T = 2π√(L/g). With g = π², T = 2π√(0.49/π²) = 2√0.49 = 1.4 s.
Answer: (A) Both Statement I and Statement II are correct
The restoring torque is τ = -mgL sin θ. Since restoring torque is proportional to sin θ rather than θ, the motion is strictly simple harmonic only when sin θ ≈ θ, which holds true for small angular displacements.
Answer: (B) 4 s
For a simple pendulum T = 2π√(L/g). With g = π², T = 2π√(4/π²) = 2√4 = 4 s.
Answer: (C) Statement I is incorrect but Statement II is correct
The restoring torque is τ = -mgL sin θ. For SHM, the restoring torque must be directly proportional to θ (τ ∝ -θ), which holds only when sin θ ≈ θ (valid for small angles). Thus, Statement I is incorrect and Statement II is correct.
Answer: (A) 2.0 × 10⁻⁴
The fractional change in length is ΔL/L = α Δθ. Since T = 2π√(L/g), the fractional change in time period is ΔT/T = (1/2)(ΔL/L) = (1/2) α Δθ = (1/2)(2.0 × 10⁻⁵)(20) = 2.0 × 10⁻⁴.