V.2 No 1 |
13 |
Transversal acoustic wave in gas | |
4. Experimental results and their analysis Two photographs of the experimental device are shown in Figures 6a and 6b: at the parallel and at normal orientation of the polarisation planes of radiator (the upper left device) and receiver (the upper right one).
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a) b)
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Fig.6. General form of experimental set when polarisation planes of radiator and receiver are parallel (a) and normal (b) to each other
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At the oscillograph screen (bottom right) you can see that
when the signal source was turned by 90o, the signal vanished. When
the radiator turning more slowly, the sinusoid at the screen slowly diminished till the
noise level, when the phase displaced by 90o. And when it displaced
by 180o, the sinusoid increased up to maximum. In turning further,
this pattern repeated. The diagrams Accurate to the error of the experiment, in both cases we can see that when the radiator turning by 180o, the signal phase varied also by 180o, and the amplitude had 8-form in the polarisation planes parallelism direction, as it is usual for a transversal wave.
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Fig.7. Experimental diagrams of amplitude Am
and phase
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Comparing the obtained results for the near and far fields, we see that when passing to that far, the phase diagram sharpens, and the amplitude diagram smears. This is caused by the fact that the spurious reflection increasingly effects on the results of experiment as the distance between the radiator and receiver increases. On the whole, the obtained results unambiguously evidence that the experimental device radiated and indicated the transversal wave in gas medium. |
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