Fluid Mechanics -4

 
 
 
 
Fluid Mechanics
Introduction

FLOATING:

When a body floats in a fluid, the magnitude Fb of the buoyant force on the body is equal to the magnitude Fg of the gravitational force on the body.

Thus, Fb = Fg (floating).

Also, Fb = mfg = Fg.

Where, mf = mass of the fluid that is displaced by the body.

APPERENT WEIGHT IN A FLUID:

If an object is placed inside a fluid then,

(Apparent weight) = (Actual weight) – (Buoyant force).

FLOW OF IDEAL FLUIDS:

An ideal fluid is incompressible and lacks viscosity, and its flow is steady and irrotational. A stream line is the path followed by an individual fluid particle.

EQUATION OF CONTINUITY:

It means that total mass of fluids going into the tube through any cross-section should be equal to the total mass coming out of the same tube from any other cross section in the same time.

                                                  Fig (6)

Thus A1V1Dt = A2V2Dt    (as shown in figure (6))

Or A1V1 = A2V2.

The product of the area of cross section and the speed remains the same at all points of a tube of flow. This is called the “equation of continuity” and expresses the law of conservation of mass in fluid dynamics.

BERNOULLI’S EQUATION:

Bernoulli’s equation relates the speed of a fluid at a point the pressure at that point and the height of that point above a reference level. It is just the application of work-energy theorem in the case of fluid flow.

We here consider the case of irrotational and steady flow of an incompressible and non viscous liquid.

According to Bernoulli’s Equation,

= Constant.

Application of Bernoulli’s Equation:

a) Hydrostatics:

If the speed of the fluid is zero every where, we get the situation of hydrostatics. Putting V1 = V2 = 0 in the Bernoulli’s equation

P1+rgh1 = P2+rgh2.

P1 - P2 = rg (h1-h2). As expected from hydrostatics.


 






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