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Fourier, J., 1822, The Analytical Theory of Heat, 1955 Dover edition of 1878 English translation.

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Article

Why q = h{ΔT}ΔT Has Been the de facto Law of Convection Heat Transfer for More Than 100 Years

1Ventuno Press, 1094 Sixth Lane N., Naples, FL 34102


American Journal of Mechanical Engineering. 2023, Vol. 11 No. 4, 141-142
DOI: 10.12691/ajme-11-4-3
Copyright © 2023 Science and Education Publishing

Cite this paper:
Eugene F. Adiutori. Why q = h{ΔT}ΔT Has Been the de facto Law of Convection Heat Transfer for More Than 100 Years. American Journal of Mechanical Engineering. 2023; 11(4):141-142. doi: 10.12691/ajme-11-4-3.

Correspondence to: Eugene  F. Adiutori, Ventuno Press, 1094 Sixth Lane N., Naples, FL 34102. Email: efadiutori@aol.com

Abstract

The purpose of engineering laws is to describe parametric behavior. Experiments indicate that h is a constant or a variable. The law of convection heat transfer cannot be q = hΔT because it states that h is always a constant. Since sometime near the beginning of the 20th century, the equation q = h{ΔT}ΔT has been the de facto law of convection heat transfer because it states that h is a constant or a variable. q = h{ΔT}ΔT is NOT dimensionally homogeneous if h is a variable because the dimension of q is not equal to the dimension of h{ΔT}ΔT. q = hΔT is not acceptable because it states that h is always a constant. q = h{ΔT}ΔT is not acceptable because it is not dimensionally homogeneous if h is a variable. A new law is required that always describes behavior, and is always dimensionally homogeneous.

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