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In , Bernoulli's principle states that an increase in the speed of a fluid occurs simultaneously with a decrease in or a decrease in the 's Bernoulli performed his experiments on liquids, so his equation in its original form is valid only for incompressible flow
"Millions of children in science classes are being asked to blow over curved pieces of paper and observe that the paper "lifts" Thus the decrease of pressure is the cause of a higher velocity

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However most people do not realize that the paper would not rise if it were flat, even though you are blowing air across the top of it at a furious rate
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The idea is that as the parcel moves along, following a streamline, as it moves into an area of higher pressure there will be higher pressure ahead higher than the pressure behind and this will exert a force on the parcel, slowing it down
ما
For a calorically perfect gas such as an ideal gas, the enthalpy is directly proportional to the temperature, and this leads to the concept of the total or stagnation temperature
Several of these explanations use the Bernoulli principle to connect the flow kinematics to the flow-induced pressures "In a demonstration sometimes wrongly described as showing lift due to pressure reduction in moving air or pressure reduction due to flow path restriction, a ball or balloon is suspended by a jet of air
The low pressure in the throat of a venturi can be explained by Bernoulli's principle; in the narrow throat, the air is moving at its fastest speed and therefore it is at its lowest pressure When we combine the head due to the flow speed and the head due to static pressure with the elevation above a reference plane, we obtain a simple relationship useful for incompressible fluids using the velocity head, elevation head, and pressure head

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In liquids — when the pressure becomes too low — occurs.

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Professor of Physics Emeritus, University of Alabama at Birmingham
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The dynamics of the upper ocean 2nd ed
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More generally, when b may vary along streamlines, it still proves a useful parameter, related to the "head" of the fluid see below