Concept:
For a pipe closed at one end, only odd harmonics are present. The resonance frequencies ($f_n$) are given by:
\[ f_n = (2n - 1) \frac{v}{4L} \quad \text{where } n = 1, 2, 3, \ldots \]
This means the allowed frequencies are odd multiples of the fundamental frequency ($f_1, 3f_1, 5f_1, \ldots$).
Step 1: Calculate the fundamental frequency ($f_1$).
Given length $L = 1$ m and speed of sound $v = 320$ ms$^{-1}$.
\[ f_1 = \frac{v}{4L} = \frac{320}{4 \times 1} = 80 \text{ Hz} \]
Step 2: Identify the allowed harmonics.
The resonance frequencies must be odd multiples of 80 Hz:
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• $f_1 = 1 \times 80 = 80 \text{ Hz}$ (Option A is possible)
• $f_2 = 3 \times 80 = 240 \text{ Hz}$ (Option C is possible)
• $f_3 = 5 \times 80 = 400 \text{ Hz}$
• $f_4 = 7 \times 80 = 560 \text{ Hz}$ (Option D is possible)
• $f_5 = 9 \times 80 = 720 \text{ Hz}$ (Option E is possible)
160 Hz is an even multiple ($2 \times 80$), which is not allowed for a pipe closed at one end.