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. 1988 Apr 1;93(2):85–144. doi: 10.6028/jres.093.010

Figure 7.

Figure 7

Perturbations to the frequency and half-width of (0,8) mode as a function of frequency, with argon in the resonator at 100 kPa. The frequency was swept by changing the temperature of the resonator, which changes the speed of sound.