An Interference Method for the Measurement of the Speed of Sound in Liquids
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In our eReader you can find the full English version of the book. Read An Interference Method for the Measurement of the Speed of Sound in Liquids Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book An Interference Method for the Measurement of the Speed of Sound in Liquids
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To quickly assess the difficulty of the text, read a short excerpt:
The vibrator was tuned by comparison with a Konig fork to 192 vibrations per second, in order that a resonator responding to that note might be used in listening at F. The object of this was to get rid of the overtones which helped to mask the minima.
The platinum point which dips into the mercury was attached to a slender brass spring, tuned to the same pitch as the vibrator in order to secure greater amplitude. The spring was about 35 mm. Long, and its amplitude at the free end was as great a...s 3 mm. , about 10 times that of the end of the vibrator bar to which it was screwed. Such an amplitude, was not only not necessary, it was not satisfactory, drops of mercury being thrown out of the cup by the platinum tip. The. Brass spring was discarded and another made whose natural period was about \y 2 times as great. This gave sufficient amplitude, about . 6 mm. , but the pitch of the vibrator rose about 12 vibrations per second when the change had been made. The first spring weighed i gram, the other .
What to read after An Interference Method for the Measurement of the Speed of Sound in Liquids?
You can find similar books in the "Read Also" column, or choose other free books by Lloyd Balderston to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
The vibrator was tuned by comparison with a Konig fork to 192 vibrations per second, in order that a resonator responding to that note might be used in listening at F. The object of this was to get rid of the overtones which helped to mask the minima.
The platinum point which dips into the mercury was attached to a slender brass spring, tuned to the same pitch as the vibrator in order to secure greater amplitude. The spring was about 35 mm. Long, and its amplitude at the free end was as great a...s 3 mm. , about 10 times that of the end of the vibrator bar to which it was screwed. Such an amplitude, was not only not necessary, it was not satisfactory, drops of mercury being thrown out of the cup by the platinum tip. The. Brass spring was discarded and another made whose natural period was about \y 2 times as great. This gave sufficient amplitude, about . 6 mm. , but the pitch of the vibrator rose about 12 vibrations per second when the change had been made. The first spring weighed i gram, the other .
What to read after An Interference Method for the Measurement of the Speed of Sound in Liquids?
You can find similar books in the "Read Also" column, or choose other free books by Lloyd Balderston to read onlineMoreLess
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