It is a principle used to model fluid dynamics in which the fluid is assumed to be both incompressible and inviscid. This theory has a wide range of applications in fluid dynamics and is often used to understand the behavior of liquids and gases.
It is a principle used to model fluid dynamics in which the fluid is assumed to be both incompressible and inviscid. This theory has a wide range of applications in fluid dynamics and is often used to understand the behavior of liquids and gases.