Convective velocity effects on a thermistor in water
Electrical powers from 5 to 150 μW were dissipated in a thermistor, causing it to rise to equilibrium temperatures above the stagnant surrounding water. Natural convection was then simulated by forced convection of water flowing up or down at known rates from 1.3 to 17 mm/min. The disturbances of th...
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Veröffentlicht in: | Journal of research of the National Bureau of Standards (1977) 1988-09, Vol.93 (5), p.603-612 |
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description | Electrical powers from 5 to 150 μW were dissipated in a thermistor, causing it to rise to equilibrium temperatures above the stagnant surrounding water. Natural convection was then simulated by forced convection of water flowing up or down at known rates from 1.3 to 17 mm/min. The disturbances of the equilibrium temperatures were measured, and are presented as effects of equivalent absorbed dose and absorbed dose rates, positive and “negative.” |
doi_str_mv | 10.6028/jres.093.152 |
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Natural convection was then simulated by forced convection of water flowing up or down at known rates from 1.3 to 17 mm/min. The disturbances of the equilibrium temperatures were measured, and are presented as effects of equivalent absorbed dose and absorbed dose rates, positive and “negative.”</abstract><pub>[Gaithersburg, MD] : U.S. Dept. of Commerce, National Institute of Standards and Technology</pub><doi>10.6028/jres.093.152</doi><tpages>10</tpages><oa>free_for_read</oa></addata></record> |
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title | Convective velocity effects on a thermistor in water |
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