As noted earlier, the heat transfer regime between conduction and convection can be considered as consisting of parallel contributions of both effects:
${\Large \frac{1}{H_{g}} = \frac{1}{H_{fm}} + \frac{1}{H_{ct}}}$
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As noted earlier, the heat transfer regime between conduction and convection can be considered as consisting of parallel contributions of both effects:
${\Large \frac{1}{H_{g}} = \frac{1}{H_{fm}} + \frac{1}{H_{ct}}}$