state and proof bernouli's theorem.
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In fluid dynamics, Bernoulli's principle states that an increase in the speed of a fluid occurs simultaneously with a decrease in pressure or a decrease in the fluid's potential energy. ...Bernoulli's principle can be derived from theprinciple of conservation of energy.
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Bernoulli's Theorem It states that the total energy (pressure energy, potential energy and kinetic energy) of an incompressible. and non-viscous fluid in steady flow through a pipe remains constant throughout the flow, provided there is no source or sink of the fluid along the length of the pipe.
proof
Let the velocity, pressure and area of the fluid column be v1, P1 and A1 at Q and v2, P2 and A2 at R. Let the volume bounded by Q and R move to S and T where QS = L1, and RT = L2. If the fluid is incompressible:
A1L1 = A2L2
The work done by the pressure difference per unit volume = gain in k.e. per unit volume + gain in p.e. per unit volume. Now:
Work done = force x distance = p x volume
Net work done per unit volume = P1 - P2
k.e. per unit volume = ½ mv2 = ½ Vρ v2 = ½ρv2 (V = 1 for unit volume)
Therefore:
k.e. gained per unit volume = ½ ρ(v22 - v12)
p.e. gained per unit volume = ρg(h2 – h1)
where h1 and h2 are the heights of Q and R above some reference level. Therefore:
P1 - P2 = ½ ρ(v12 – v22) + ρg(h2 - h1)
P1 + ½ ρv12 + ρgh1 = P2 + ½ ρv22 + rgh2
Therefore:
P + ½ ρv2 + ρgh is a constant
For a horizontal tube h1 = h2 and so we have:
P + ½ ρv2 = a constant
This is Bernoulli's theorem You can see that if there is a increase in velocity there must be a decrease of pressure and vice versa.
No fluid is totally incompressible but in practice the general qualitative assumptions still hold for real fluids.
proof
Let the velocity, pressure and area of the fluid column be v1, P1 and A1 at Q and v2, P2 and A2 at R. Let the volume bounded by Q and R move to S and T where QS = L1, and RT = L2. If the fluid is incompressible:
A1L1 = A2L2
The work done by the pressure difference per unit volume = gain in k.e. per unit volume + gain in p.e. per unit volume. Now:
Work done = force x distance = p x volume
Net work done per unit volume = P1 - P2
k.e. per unit volume = ½ mv2 = ½ Vρ v2 = ½ρv2 (V = 1 for unit volume)
Therefore:
k.e. gained per unit volume = ½ ρ(v22 - v12)
p.e. gained per unit volume = ρg(h2 – h1)
where h1 and h2 are the heights of Q and R above some reference level. Therefore:
P1 - P2 = ½ ρ(v12 – v22) + ρg(h2 - h1)
P1 + ½ ρv12 + ρgh1 = P2 + ½ ρv22 + rgh2
Therefore:
P + ½ ρv2 + ρgh is a constant
For a horizontal tube h1 = h2 and so we have:
P + ½ ρv2 = a constant
This is Bernoulli's theorem You can see that if there is a increase in velocity there must be a decrease of pressure and vice versa.
No fluid is totally incompressible but in practice the general qualitative assumptions still hold for real fluids.
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