D'Alembert's principle is a reformulation of Newton's second law of motion (\(\vec{F} = m\vec{a}\)).
It states that the vector sum of the external forces (\(\vec{F}\)) acting on a body and the inertial force (or fictitious force) \( -m\vec{a} \) is zero.
$$ \sum \vec{F} - m\vec{a} = 0 $$
By introducing the inertial force (\(-m\vec{a}\)), which acts opposite to the acceleration, the dynamic problem (\(\sum \vec{F} = m\vec{a}\)) is transformed into an equivalent problem of static equilibrium (\(\sum \vec{F}_{effective} = 0\)).
This allows methods of statics to be applied to problems involving motion (dynamics), often simplifying the analysis, particularly in complex systems.
It is fundamental in mechanics, not specifically fluid dynamics, chemical reactions, or heat transfer.