State and prove Torricelli’s theorem.

Statement: The velocity of efflux of the liquid through an orifice is equal to the velocity which a body would attain in free fall from the surface of liquid to orifice.


Statement: The velocity of efflux of the liquid through an orifice is

Proof: Consider a tank containing an ideal liquid of density ρ and having a narrow orifice at L. Let the tank be very wide as compared to orifice so that velocity of its free surface can be taken zero. Let v be velocity of efflux. The pressure at free surface M of liquid and at orifice L is atmospheric i.e. P and let h be the height of liquid above orifice. Applying Bernoulli's theorem at L and M,


Statement: The velocity of efflux of the liquid through an orifice is
Hence velocity of efflux of liquid is equal to velocity of free falling body.
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State and prove Bernoulli's theorem.

Statement: For the streamline flow of non-viscous and incompressible liquid, the sum of potential energy, kinetic energy and pressure energy is constant.


Statement: For the streamline flow of non-viscous and incompressible

Proof: Let us consider the ideal liquid of density ρ flowing through the pipe LM of varying cross-section. Let P1 and P2 be the pressures at ends L and M and A1 and A2 be the areas of cross-sections at ends L and M respectively. Let the liquid enter with velocity V1 and leave with velocity v2. Let A1 > A2. By equation of continuity,


Statement: For the streamline flow of non-viscous and incompressible

Statement: For the streamline flow of non-viscous and incompressible
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What is the principle of venturimeter? Derive an expression for the rate of flow of liquid through it.


Venturimeter is based on Bernoulli's theorem. It consists of a two truncated tubes connected by a pipe at narrow ends. The pipe connecting the two tubes is called throat as shown in figure.

The venturimeter tube is positioned horizontally and the liquid is made to enter in it at end A and after passing through throat BC, it leaves tube at end D. Let at A, the area of cross-section of tube be a1, pressure of liquid be P1 and velocity be v1 And at the throat, the area of cross-section of tube be a2 pressure of liquid be P2 and velocity be v2



Venturimeter is based on Bernoulli's theorem. It consists of a two tr

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Why does deep water run slow?


Let water be flowing in a river of width b. Let d\ and d1 (d1 < d2) be the depth of river at two different places in the river and v1 and v2 be the velocities of water at those two places respectively. Therefore, according to the equation of continuity,


Let water be flowing in a river of width b. Let d\ and d1 (d1 <

That is where depth is more speed is less and vice versa. Hence deep water runs slow and shallow water runs fast.
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Derive equation of continuity for steady flow of incompressible liquid.

Let us consider that a liquid is flowing through a pipe of varying cross-section as shown in figure.


Let us consider that a liquid is flowing through a pipe of varying cr

Let the liquid enter at A with velocity v1 where area of cross-section is a1 and exit at end B with velocity v2 where area of cross-section is a2.Let ρ1 and ρ2 be the densities of liquid at ends A and B respectively.

Now the volume of liquid that enters in one second at end A is,

V1 = a1 v1

Mass of liquid entering per second at end A is,

Similarly the mass of liquid leaving per second at end B is,

m2 = a2v2ρ2

If there is no source or sink of liquid, then mass of liquid that enters at end A in one second is equal to the mass of liquid that leave in one second, i.e.

a1 v1 p1 = a2 vp2

If the liquid is incompressible, then ρ1 = ρ2. Therefore equation (1) reduces to

a1v1= a2v2 ......(2)

This equation is called equation of continuity.

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