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Cooling sound during

Many cells, especially bacteria, yeast, etc., require very drastic measures to disrupt them and various cell disintegrators are available for this purpose. Ultrasonic vibrations cause the formation of minute bubbles, a phenomenon known as cavitation, which is caused by the extreme variations in pressure generated by the sound waves, although the generation of heat may cause problems unless the samples are cooled frequently during the treatment. An additional... [Pg.296]

Fig. 6. Speed of sound during cooling of a sample of confectionary coating fat at a shear rate of 0 ( ) or 10O s ( ). Fig. 6. Speed of sound during cooling of a sample of confectionary coating fat at a shear rate of 0 ( ) or 10O s ( ).
Fig. 3. Ultrasonic reflectance amplitude from the interface between a piece of Plexiglas and sample of confectionary coating fat during cooling. As the sample crystallized, it became more acoustically similar to the Plexiglas and less sound was reflected. Fig. 3. Ultrasonic reflectance amplitude from the interface between a piece of Plexiglas and sample of confectionary coating fat during cooling. As the sample crystallized, it became more acoustically similar to the Plexiglas and less sound was reflected.
During operations, conditions in the detonation chamber are monitored using an air-cooled camera located in a tube that protrudes into the chamber. A slight negative pressure is maintained in the chamber to enable detection of the pressure pulse that takes place when a munition detonates. A microphone is used to detect the sound of a detonation, and vibration of the chamber is also recorded. [Pg.64]

Worldwide a large amount of experience has been accumulated during development, licensing, construction and operation of gas-cooled reactors. The experience forms a sound basis for programmes which are underway in several countries to develop advanced high temperature reactors for electric power generation and for process heat. [Pg.258]

Alvarenga et al. [66] introduced the use of Brillouin scattering to measure the sound velocity in stretched liquid water during cooling. They reported tensions beyond —100 MPa at 20°C. The pressure was calculated from the change in sound velocity before and after cavitation, assuming a linear relation based on positive pressure data. [Pg.65]

Although the thermal conductivity, specific heat, and sound velocity temperature dependence for both samples are similar, the heat release shows different time dependences as well as different values in apparent contradiction with the other measured low-temperature properties. Taking into account the internal friction results, it is tempting to correlate the differences in the heat release between both samples to the difference in the contribution of thermally activated processes in the relaxation of the tunneling states during the cooling process. [Pg.65]

Laplace, Pierre Simon (1749-1827) A French professor of mathematics noted for his contribution to mathematics. Lapiace was the son of a farm iabourer who owed his education to some rich neighbours. He soived many probiems concerning the motion of the solar system. He also worked on surface tension and, with Antoine Lavoisier (1743-94), did work on the measurement of the heat produced during chemical changes. In 1822 he persuaded the French Academy to carry out experiments to measure the velocity of sound over a distance of eleven miles by firing cannons. The result confirmed his belief that when sound waves pass, the air cools as it expands and heats up as it contracts. [Pg.214]


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