Govt. Exams
Entrance Exams
For a tube closed at one end (water surface), first resonance occurs at L = λ/4. Given f = 512 Hz, v = 340 m/s, λ = v/f = 340/512 ≈ 0.664 m. So λ/4 ≈ 0.166 m = 16.6 cm. The effective length includes end correction (≈1 cm for open end), so L_eff = 16.2 + 1 = 17.2 cm, which equals λ/4 within measurement precision.
From y = 0.02sin(50πt - 4πx), comparing with y = Asin(ωt - kx): ω = 50π rad/s, k = 4π rad/m. Wavelength λ = 2π/k = 2π/(4π) = 0.5 m. Wave velocity v = ω/k = 50π/(4π) = 12.5 m/s.
When a wave reflects from a fixed (denser) end, it undergoes a phase change of π radians or 180°
Original: A₀ = A + A = 2A, so A = A₀/2. New amplitude = A₀/2 + A₀/4 = 3A₀/4 (if each gets halved) or A + A/2 = 3A/2 = 3A₀/4. Actually, new = A₀/2 + A₀/2 = A₀ or (A₀/2)/2 + A₀/2 = 3A₀/4
Intensity ∝ 1/r². I₂/I₁ = (r₁/r₂)² = (1/10)² = 1/100. I₂ = 10⁻⁸/100 = 10⁻¹⁰ W/m²
Phase difference = (2π/λ) × path difference = (2π/20) × 10 = π radian
A closed organ pipe resonates at odd multiples: f₁, 3f₁, 5f₁... The next resonance after 200 Hz is 3×200 = 600 Hz
From y = A cos(kx) sin(ωt), we have k = π, so λ = 2π/k = 2π/π = 2 cm
Using Snell's law: n₁sin(θ₁) = n₂sin(θ₂). 1.5 × sin(30°) = 1 × sin(θ₂). θ₂ = 48.75°
Beat frequency = |f₁ - f₂| = |250 - 254| = 4 Hz