Abstract
A generalized theory of 3He-A phase superfIuid is establisped, which can comprise the Khalatnikov-Lebedev’s theory treated as a special case. The starting point of this work is the Zilsel’s principle in which the density of the superfluid component is defined as an independent variable. It has the advantage of including naturally the “heating effect” of 3He-A superfluid liquid, whereby overcoming the difficulties encountered in Khalatnikov-Lebedev’s theory.
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