The total energy of each particle at various places in the case of perfect incompressible fluid flowing in continuous stream
Remains constant
When we talk about a perfect incompressible fluid flowing in a continuous stream, a fundamental principle of fluid dynamics comes into play: Bernoulli's principle. This principle is essentially an application of the conservation of energy for ideal fluids in steady flow.
Bernoulli's principle states that for a non-viscous, incompressible fluid in steady flow, the sum of pressure energy per unit volume, kinetic energy per unit volume, and potential energy per unit volume is constant at every point along a streamline.
This constant sum represents the total energy per unit volume of the fluid. For each individual particle within this ideal fluid flow, its total energy, which is the sum of:
remains the same as it moves along its path (a streamline).
The question describes a "perfect incompressible fluid flowing in continuous stream". This perfectly matches the conditions under which Bernoulli's principle is applicable. 'Perfect' implies non-viscous, and 'incompressible' means the density doesn't change. 'Continuous stream' implies steady flow along streamlines.
Therefore, according to Bernoulli's principle, the total energy of each particle in such a fluid, at various places along its flow path, does not change.
For a perfect incompressible fluid flowing in a continuous stream, the total energy of each particle at various places remains constant because the flow adheres to Bernoulli's principle, which is a statement of energy conservation for ideal fluids.
The coefficient of contraction Cc for an orifice can be determined using other coefficients; discharge and velocity Cv by the relation.
When Venturimeter is inclined, then for a given flow it will show
The energy loss in flow through nozzle as compared to venturimeter is
A pitot static tube is used to measure the velocity of water in a pipe. The stagnation pressure head is 6 m and static pressure head is 5 m. Calculate the velocity of flow assuming the coefficient if tube equal to 0.98.
Navier–stokes equation applies to: