Abstract
INTERNAL calorimetry1, developed for the measurement of blood flow, is basically a method for thermal conductivity determination. It uses a fine-gauge heated thermocouple embedded in the organ or medium under examination. In simple media a steady heating current applied to the filament raises the temperature recorded by the thermocouple. Temperature equilibration is rapid. Heat exchanges2 are governed by Carslaw's equation3: I2R = 4π.r.θ.k, where k is the thermal conductivity of the medium, I the heating current, R the resistance of the heater, r the radius of a thermodynamically equivalent sphere and θ the temperature increment. Thus the relation between I2 and θ is linear when k is constant; 4πr/R is a constant for any given recorder and constitutes its standardization factor (F), the experimental determination of which has been fully described elsewhere4.
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References
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Carslaw, H. S., “The Mathematical Theory of the Conduction of Heat in Solids” (London: Macmillan and Co., Ltd., 1921).
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Read, J. H., and Lloyd, D. M. G., Trans. Farad. Soc., 44, 721 (1948).
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HAIGH, A. Thermal Conductivity Measurements on Inert Media using Internal Calorimetry. Nature 173, 493–494 (1954). https://doi.org/10.1038/173493b0
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DOI: https://doi.org/10.1038/173493b0