Bernouli's theorem holds for incompressible, non-viscous fluids. How is this relationship changed when the viscosity of the fluid is not negligible?

Statement-1 : Bernoulli’s theorem holds for incompressible, non-viscous fluids. Statement-2 : The factor (v^(2))/(2g) is called velocity head.

A: Bernoulli's theorem holds good only for non viscous and incompressible liquid. R: Bernoulli’s theorem is based on the conservation of energy

The pressure of an imcompressible & non - viscous fluid also depends upon the velocity of flow at that point .

Obtain the equation of continuity for the incompressible non - viscous fluid having a steady flow through a pipe.

A cubical block of side a and density rho slides over a fixed inclined plane with constant velocity v . There is a thin film of viscous fluid of thickness t between the plane and the block. Then the coefficient of viscosity of the thin film will be: (Acceleration due to gravity is g)

Human blood is a viscous fluid. This viscosity is due to

A spherical ball of density rho and radius 0.003m is dropped into a tube containing a viscous fluid up to the 0 cm mark as shown in the figure. Viscosity of the fluid =1.26N-s//m^(2) and its density rho_(L)=(rho)/(2)=1260kg//m^(3) . Assume that the ball reaches a terminal speed at 10cm mark. The time taken by the ball to travel the distance between the 10cm and 20cm mark is (g=10m//s^(2))

Bernouli's equation for a steady streamline flow of a non-viscous incompressible fluid expresses the principle of

The loss of pressure when a fluid flows through a pipe is give by P = krho^(a)l V^(b)d^(c) mu where d and l are diameter and length of the pipe respectively, rho,d and mu are the mass, density and coefficient of viscosity of the fluid, V is the mean velocity of flow through the pipe and k is a numerical constant. Find the values of a, b and c.