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Τι (ποιος) είναι incompressible liquid - ορισμός
![[[Surface wave]]s in water](https://commons.wikimedia.org/wiki/Special:FilePath/2006-01-14 Surface waves.jpg?width=200 "[[Surface wave]]s in water")
![A [[lava lamp]] contains two immiscible liquids (a molten wax and a watery solution) which add movement due to convection. In addition to the top surface, surfaces also form between the liquids, requiring a tension breaker to recombine the wax droplets at the bottom.](https://commons.wikimedia.org/wiki/Special:FilePath/Blue Lava lamp.JPG?width=200 "A [[lava lamp]] contains two immiscible liquids (a molten wax and a watery solution) which add movement due to convection. In addition to the top surface, surfaces also form between the liquids, requiring a tension breaker to recombine the wax droplets at the bottom.")
![Lennard-Jones model fluid]].](https://commons.wikimedia.org/wiki/Special:FilePath/Lennard-Jones Radial Distribution Function.svg?width=200 "Lennard-Jones model fluid]].")
![deposition]] can occur.](https://commons.wikimedia.org/wiki/Special:FilePath/Phase-diag2.svg?width=200 "deposition]] can occur.")
![A simulation of [[viscosity]]. The fluid on the left has a lower viscosity and Newtonian behavior while the liquid on the right has higher viscosity and non-Newtonian behavior.](https://commons.wikimedia.org/wiki/Special:FilePath/Viscosities.gif?width=200 "A simulation of [[viscosity]]. The fluid on the left has a lower viscosity and Newtonian behavior while the liquid on the right has higher viscosity and non-Newtonian behavior.")
Βικιπαίδεια
In fluid mechanics or more generally continuum mechanics, incompressible flow (isochoric flow) refers to a flow in which the material density is constant within a fluid parcel—an infinitesimal volume that moves with the flow velocity. An equivalent statement that implies incompressibility is that the divergence of the flow velocity is zero (see the derivation below, which illustrates why these conditions are equivalent).
Incompressible flow does not imply that the fluid itself is incompressible. It is shown in the derivation below that (under the right conditions) even compressible fluids can – to a good approximation – be modelled as an incompressible flow. Incompressible flow implies that the density remains constant within a parcel of fluid that moves with the flow velocity.
