Statement :
When an incompressible and
non-viscous liquid (or gas) flows in streamlined motion from one place to
another, then at every point of its path the total energy per unit volume
is constant.
That is= constant.
Bernoulli’s Theorem:
=constant
Thus, Bernoulli’s theorem is in one
way the principle of conservation of energy for a flowing liquid (or gas).
Bernoulli’s Equation:
Let
us focus our attention on the motion of the shaded region. This its our
“system”. The lower cylindrical element of fluid of length A1 is at height y1 which moves with
speed v1After some time, the
leading section of our system fills the upper cylinder of fluid of length and area A2 at
height y2 and is then moving with speed v2.
A pressure force F1 acts on the lower part of the cylindrical tube
towards right and pressure force F2 acts on the upper part of the cylindrical tube
towards left. The net work done on the system F1 and F2 is
Where we have used the relations and . The net effect of
the motion of the system is to raise the height of the lower cylinder of
mass and to change its speed. The
changes in the potential and kinetic energies are
Since the density is, we have
Since the points 1 and 2 can be
chosen arbitrarily, we can express this result as Bernoulli’s Equation
= constant
It is applied to all points along a
streamline in a nonviscous, incompressible and irrotational fluid.
Example : Figure shows a liquid of density 1200
kg/m3 flowing steadily in a tube of varying
cross-section. The cross-section at a point A is 1.0 cm2 and that at B is 20 mm2, the points A and B
are in the same horizontal plane. The speed of the liquid at A is 10 cm/s.
Calculate the difference in pressures at A and B.
Solution : From equation of continuity,
the speed n2 at B is given by,
A1n1 = A2n2
By Bernoulli’s
equation,
Here h1 = h2.
Thus,
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