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    Bernoulli's principleFrom Wikipedia, the free encyclopedia

    This article is about Bernoulli's principle and Bernoulli's equation in fluid dynamics. For Bernoulli's theorem

    in probability, seelaw of large numbers. For an unrelated topic inordinary differential equations,seeBernoulli differential equation.

    A flow of air into aventuri meter. The kinetic energy increases at the expense of thefluid pressure, as shown by the

    difference in height of the two columns of water.

    Continuum mechanics

    Laws[show]

    Solid mechanics[show]

    Fluid mechanics[show]

    Rheology[show]

    Scientists[show]

    V

    T

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    E

    Influid dynamics,Bernoulli's principle states that for aninviscid flow, an increase in the speed of the fluid

    occurs simultaneously with a decrease inpressureor a decrease in thefluid'spotential

    energy.[1][2]

    Bernoulli's principle is named after the Swiss scientist Daniel Bernoulliwho published his

    principle in his book Hydrodynamica in 1738.[3]

    Bernoulli's principle can be applied to various types of fluid flow, resulting in what is loosely denoted

    as Bernoulli's equation. In fact, there are different forms of the Bernoulli equation for different types of

    flow. The simple form of Bernoulli's principle is valid forincompressible flows(e.g. mostliquidflows) and

    also forcompressible flows(e.g.gases) moving at lowMach numbers(usually less than 0.3). More

    advanced forms may in some cases be applied to compressible flows at higherMach numbers(seethe

    derivations of the Bernoulli equation).

    An inviscid flow is the flow of anideal fluidthat is assumed to have noviscosityIn most flows of liquids, and of gases at lowMach number, thedensityof a fluid parcel can be

    considered to be constant, regardless of pressure variations in the flow. Therefore, the fluid can be

    considered to be incompressible and these flows are called incompressible flow. Bernoulli performed

    his experiments on liquids, so his equation in its original form is valid only for incompressible flow. A

    common form of Bernoulli's equation, valid at anyarbitrarypoint along astreamline, is:

    (

    A

    )

    where:

    is the fluid flowspeedat a point on a streamline,

    is theacceleration due to gravity,

    is theelevationof the point above a reference plane, with the positive z-direction pointing

    upward so in the direction opposite to the gravitational acceleration,

    is thepressureat the chosen point, and

    is thedensityof the fluid at all points in the fluid.

    Forconservative forcefields, Bernoulli's equation can be generalized as:[8]

    where is theforce potentialat the point considered on the

    streamline. E.g. for the Earth's gravity = gz.

    The following two assumptions must be met for this Bernoulli equation

    to apply:[8]

    the flow must be incompressible even though pressure varies,the density must remain constant along a streamline;

    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    friction by viscous forces has to be negligible.

    By multiplying with the fluid density , equation (A) can be rewritten as:

    or:

    where:

    isdynamic pressure,

    is thepiezometric headorhydraulic head(the sum of the elevation zand

    thepressure head)[9][10]

    and

    is thetotal pressure(the sum of the static pressurep and dynamic

    pressure q).[11]

    The constant in the Bernoulli equation can be

    normalised. A common approach is in terms

    oftotal head orenergy headH:

    Bernoulli Equation

    The Bernoulli Equation can be considered to be a statement of theconservation ofenergyprinciple appropriate for flowing fluids. The qualitative behavior that isusually labeled with the term "Bernoulli effect" is the lowering of fluid pressure inregions where the flow velocity is increased. This lowering of pressure in a

    constriction of a flow path may seem counterintuitive, but seems less so when youconsider pressure to beenergy density. In the high velocity flow through the

    constriction, kinetic energy must increase at the expense of pressure energy.

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