@article{ajme20231143,
author={Adiutori, Eugene F.},
title={Why <i>q = h{ĶĪT}ĶĪT</i> Has Been the <i>de facto</i> Law of Convection Heat Transfer for More Than 100 Years},
journal={American Journal of Mechanical Engineering},
volume={11},
number={4},
pages={141--142},
year={2023},
url={http://pubs.sciepub.com/ajme/11/4/3},
issn={2328-4110},
abstract={The purpose of engineering laws is to describe parametric behavior. Experiments indicate that <i>h</i> is a constant or a <i>variable</i>. The law of convection heat transfer <i>cannot</i> be <i>q = hĶĪT</i> because it states that <i>h</i> is <i>always</i> a <i>constant</i>. Since sometime near the beginning of the 20<SUP>th</SUP> century, the equation <i>q = h{ĶĪT}ĶĪT </i>has been the de facto law of convection heat transfer because it states that <i>h</i> is a constant or a <i>variable</i>. <i>q = h{ĶĪT}ĶĪT</i> is NOT dimensionally homogeneous if <i>h</i> is a variable because the dimension of <i>q</i> is not equal to the dimension of <i>h{ĶĪT}ĶĪT</i>. <i>q = hĶĪT</i> is not acceptable because it states that <i>h</i> is <i>always</i> a constant. <i>q = h{ĶĪT}ĶĪT</i> is not acceptable because it is <i>not</i> dimensionally homogeneous if <i>h</i> is a variable. A new law is required that always describes behavior, and is <i>always</i> dimensionally homogeneous.},
doi={10.12691/ajme-11-4-3}
publisher={Science and Education Publishing}
}
