Resonance ColumnJEE Main

Measure the speed of sound with a tuning fork — interactive Physics simulation for IIT-JEE.

Concept

An air column closed at the bottom (by water) resonates with a tuning fork when its length fits an odd number of quarter wavelengths — a node at the water, an antinode near the open top. Raising the water and hearing the loudness peak twice gives two lengths whose difference is exactly λ/2\lambda/2, eliminating the messy end effects.

Key formula

l1+e=λ4,l2+e=3λ4    v=2f(l2l1),e0.3dl_1 + e = \frac{\lambda}{4}, \qquad l_2 + e = \frac{3\lambda}{4} \;\Rightarrow\; v = 2f(l_2 - l_1), \qquad e \approx 0.3d

Derivation

Closed pipe modes: L=(2n1)λ/4L = (2n-1)\lambda/4. The antinode actually forms slightly ABOVE the tube mouth — the end correction e.

Subtracting the two resonance conditions kills e: l2l1=λ/2l_2 - l_1 = \lambda/2. Then v=fλ=2f(l2l1)v = f\lambda = 2f(l_2-l_1) — a clean lab measurement. Back-substituting gives e=(l23l1)/2e = (l_2 - 3l_1)/2.

Scenarios to explore

  • Resonance Column — Measure the speed of sound with a tuning fork & water column.

Real-world applications

  • Standard JEE/NEET lab experiment for v_sound.
  • Organ pipe & wind-instrument tuning.
  • Acoustic impedance tubes in materials testing.

JEE exam tips

  • v = 2f(l₂ − l₁) needs no end correction — that's the whole point of two readings.
  • Third resonance sits at l₃ = l₁ + λ (≈ 5λ/4 − e).
  • Temperature: v ∝ √T — quote v at the lab temperature.

Common mistakes

  • Using l₂ − l₁ = λ (it's λ/2).
  • Forgetting e when computing λ from a SINGLE resonance length.
  • Expecting a resonance at l₂ = 2l₁ — closed pipes have only odd multiples.

Exam traps to avoid

  • The water surface is always a displacement NODE (pressure antinode).
  • e = (l₂ − 3l₁)/2 comes straight from the two equations — derivable, no memorising.