Fast Fourier Transformed Acoustic Resonances With Sonic Transform
Fast Fourier Transformed Acoustic Resonances With Sonic Transform
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42 43 Note that ST transforms shown in Figures 4-5 and 4-6 correctly recover the input sonic speeds (350 m/s and 150 m/s) .
Figure 4-7 is an experimentally acquired waveform of the resonances of argon at a low temperature (-31.56oC) in a spherical cavity with a 3.000 inch radius. The experimental conditions are given in Table 4-1. An expanded view of a section of Figure 4-7 is given in Figure 4-8 to show the resolution with which the waveform is acquired in other regions. The FFT of the wavefor...m of Figure 4-7 is shown in Figure 4-9 and the relevant physical and computational parameters are given in Table 4-2. As seen in Figure 4-9, the baseline is not very stable in the region of 10,000 Hz.
An expanded view of this region is shown in Figure 4-10.
Several STs were performed on the data in Figure 4-9 using different numbers of roots. The resulting ST weights employing the first 21 roots are shown in Figure 4-11 with an expanded view of the region that contains the known speed of sound in argon shown in Figure 4-12.
What to read after Fast Fourier Transformed Acoustic Resonances With Sonic Transform?
You can find similar books in the "Read Also" column, or choose other free books by Mcgill, Kenneth C., 1957- to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
42 43 Note that ST transforms shown in Figures 4-5 and 4-6 correctly recover the input sonic speeds (350 m/s and 150 m/s) .
Figure 4-7 is an experimentally acquired waveform of the resonances of argon at a low temperature (-31.56oC) in a spherical cavity with a 3.000 inch radius. The experimental conditions are given in Table 4-1. An expanded view of a section of Figure 4-7 is given in Figure 4-8 to show the resolution with which the waveform is acquired in other regions. The FFT of the wavefor...m of Figure 4-7 is shown in Figure 4-9 and the relevant physical and computational parameters are given in Table 4-2. As seen in Figure 4-9, the baseline is not very stable in the region of 10,000 Hz.
An expanded view of this region is shown in Figure 4-10.
Several STs were performed on the data in Figure 4-9 using different numbers of roots. The resulting ST weights employing the first 21 roots are shown in Figure 4-11 with an expanded view of the region that contains the known speed of sound in argon shown in Figure 4-12.
What to read after Fast Fourier Transformed Acoustic Resonances With Sonic Transform?
You can find similar books in the "Read Also" column, or choose other free books by Mcgill, Kenneth C., 1957- to read onlineMoreLess
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