In a resonance tube closed at one end, the fundamental frequency corresponds to a resonance at the first harmonic (where the tube behaves like a pipe with a closed end). The lengths \( l_1 \) and \( l_2 \) correspond to successive resonances, and we use this information to calculate the frequency of sound.
The difference in lengths \( \Delta l \) between two resonant positions corresponds to half of the wavelength of the sound. Thus, we have:
\[
\Delta l = l_2 - l_1 = 200 \, \text{cm} - 120 \, \text{cm} = 80 \, \text{cm} = 0.8 \, \text{m}
\]
This represents half the wavelength, so the full wavelength \( \lambda \) is:
\[
\lambda = 2 \times 0.8 \, \text{m} = 1.6 \, \text{m}
\]
Now, we use the wave equation \( v_s = f \lambda \), where \( v_s \) is the speed of sound and \( f \) is the frequency of the sound. Solving for \( f \):
\[
f = \frac{v_s}{\lambda} = \frac{340 \, \text{m/s}}{1.6 \, \text{m}} = 212.5 \, \text{Hz}
\]
Thus, the frequency of the sound is 1000 Hz.
Therefore, the correct answer is (B) 1000 Hz.