Narrow the pipe and watch what happens to the fluid. From the continuity equation the flow speed rises at the narrow point, and from Bernoulli's principle p+½ρv²=const a rising speed means a drop in pressure. This is how an aerofoil and an atomiser work.

I'll give you a target speed in the constriction — tune the pipe cross-section to reach it. S·v = const.
What just happened?
You narrowed the pipe, the fluid stream sped up and the static pressure dropped. It is not magic — it is a direct consequence of energy conservation for a flowing fluid.
Continuity equation (incompressible fluid):
— the same amount of fluid passes through every pipe cross-section in the same time. A smaller cross-section ⇒ a higher speed . That is why the streamlines bunch up in the constriction.
Bernoulli's equation (horizontal pipe):
— the sum of the static pressure and the dynamic pressure is constant. As the speed rises, the "dynamic" term takes more and more, so the static pressure must drop. — the fluid density.
What does this mean in practice?
Fast flow = low pressure. This is how a carburettor and an atomiser work (the Venturi effect), how an aircraft gains lift, and why two boats sailing close together are "sucked" toward each other.
Why you need this for the exam:
In pipe-constriction problems, first use to find the speed in the constriction, then to compute the pressure. Trick: where it is tighter and faster, the pressure is lower.
Remember: faster-flowing fluid exerts lower pressure — p + ½ρv² = const. In the constriction the speed rises and the pressure drops.
For an incompressible fluid the product of cross-sectional area and speed is constant: In a constriction (smaller ) the speed must rise.
The sum of the static and dynamic pressure along a streamline is constant (at one level): Since rises in the constriction, the static pressure must drop.
Aerofoil lift, the carburettor, the atomiser, the Venturi tube, a "curved" ball.
Notation: — pipe cross-sectional area, — flow speed, — static pressure, — fluid density, — dynamic pressure.
Because the sum of the static and dynamic pressure is constant (p+½ρv²=const); as the speed v rises, the static pressure p must drop.
From the continuity equation S·v=const — a smaller cross-section S forces a higher speed v so that the flow is conserved.
Aerofoil lift, the carburettor, the atomiser, the Venturi tube, a "curved" ball.
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