LASER FLASH EQUIPMENT
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| Thermal diffusivity range: 10-3 to 1 cm2 /s |
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| Samples under study: | |||||||||||||||||||||
| Rocks | |||||||||||||||||||||
| Temperature Range: | |||||||||||||||||||||
| Room temperature up to 2200 ºC. (High temperature furnace.) | |||||||||||||||||||||
| Room temperature down to -150 ºC. (Cryogenic unit.) | |||||||||||||||||||||
| Uncertainty: | |||||||||||||||||||||
| +/- 5 %. | |||||||||||||||||||||
| Calibration of the instrument: | Some Results: | ||||||||||||||||||||
| Poco Graphite AXM-5QL; |
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| Pyroceram 9606; | |||||||||||||||||||||
| Fused silica; | |||||||||||||||||||||
| Copper; | |||||||||||||||||||||
| Austenitic stainless steel. | |||||||||||||||||||||
| Methodology: | |||||||||||||||||||||
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The
laser flash is based on optical methods with a strong impact, used for the
measurement of the thermal diffusivity of solids. The success of this
method owes, essentially, not only to the reduced time interval necessary
for the realisation of the measurements, but also because of the
simplicity of the sample, the ability to study very different substances
and the possibility to work at high temperatures.
Conceptually, the laser flash method is very simple. A small disc
of the material to be studied is kept at a constant temperature and
thermally isolated from the surroundings. One of its faces is subjected to
fast axial heat pulse. The temperature of a certain point on the rear face
of the sample is monitored as a function of time. This assumption is valid
in the case of homogeneous materials. The determination of the thermal diffusivity can be made in several ways. In the simplest case, the time that the rear face takes to reach a half of its maximum value is measured. |
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Instrument characteristics: |
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| (Financed by the PRAXIS Program - FCT) | |||||||||||||||||||||
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ANTER CORPORATION (USA)
MODEL FL5000 |
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| Photos (click to view the full size): | |||||||||||||||||||||
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Lab: |
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Rock Samples: |
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