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Stage 3 – Page 2 : Standing Waves on a Stretched String
1️⃣ Fixed End & Free End – Boundary Conditions
📌 Fixed End
- Displacement = 0
- Always a Node
📌 Free End
- Slope = 0
- Always an Antinode
⚠ Boundary conditions decide allowed wavelengths.
2️⃣ String Fixed at Both Ends
Let length of string = L
Allowed Wavelengths
λₙ = 2L / n (n = 1, 2, 3, …)
Allowed Frequencies
fₙ = n (v / 2L)
Where wave speed:
v = √(T / μ)
- T = tension in string
- μ = mass per unit length
3️⃣ Harmonics on Fixed–Fixed String
- n = 1 → Fundamental (1st harmonic)
- n = 2 → 2nd harmonic
- n = 3 → 3rd harmonic
- All harmonics are present
✔ Fundamental frequency is the lowest possible frequency.
4️⃣ String Fixed at One End & Free at Other End
Length of string = L
Allowed Wavelengths
λₙ = 4L / (2n − 1)
Allowed Frequencies
fₙ = (2n − 1) (v / 4L)
- n = 1 → Fundamental
- n = 2 → 3rd harmonic
- n = 3 → 5th harmonic
⚠ Even harmonics are absent.
5️⃣ Comparison Table (Very Important)
| Feature | Fixed–Fixed String | Fixed–Free String |
|---|---|---|
| Ends | Node–Node | Node–Antinode |
| Harmonics | All present | Only odd |
| Fundamental λ | 2L | 4L |
| Fundamental f | v / 2L | v / 4L |
6️⃣ Effect of Physical Parameters
- Increase tension → frequency increases
- Increase mass density → frequency decreases
- Frequency ∝ √T
- Frequency ∝ 1/√μ
7️⃣ JEE Advanced Concept Traps
- Mixing fixed–free with fixed–fixed formulas
- Wrong harmonic counting
- Forgetting √T relation
- Using λ instead of L directly
🎯 Final Takeaway
✔ Boundary conditions decide wave pattern ✔ Harmonics differ for different end conditions ✔ Formulas must be chosen carefully
Stage 3 – Page 2 Completed Successfully ✅
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