← The collection

Bernoulli’s Principle.

Narrow an ideal horizontal pipe and compare speed with static pressure.

Interactive experimentintuitiveField note ·
INTERACTIVE EXPERIMENT / P08

Bernoulli’s Principle

Narrow an ideal horizontal pipe and compare speed with static pressure.

TEST THE MECHANISM

Water flows steadily through a horizontal ideal pipe. The first area is 4 cm² and pressure 400 kPa. Change the second area without changing the selected volume flow.

18
0.22
4 cm² →1 cm² →
First speed (m/s)
2.50
Second speed (m/s)
10.00
Second ideal pressure (kPa)
353.13
Flow at both sections (L/s)
1.00

Continuity fixes area times velocity; Bernoulli balances pressure and kinetic energy at equal height. The pipe is schematic. Viscosity, turbulence, pumps and energy losses are omitted.

Steady incompressible inviscid flow without pumps is assumed. Geometry is schematic; turbulence, friction and energy losses are not predicted.

THE SHORT VERSION

Bernoulli’s Principle, explained.

Bernoulli’s principle balances pressure, kinetic and gravitational energy along a streamline under specified ideal-flow conditions.

01 / THE MECHANISM

Why it happens

Fixed volume flow makes velocity inversely proportional to cross-section area. At equal height, pressure difference is half the water density times the difference in squared speeds.

Bernoulli’s principle balances pressure, kinetic and gravitational energy along a streamline under specified ideal-flow conditions.

Read the result

The same selected volume flow passes both sections. The higher local velocity comes from smaller area, with pressure changing to preserve the ideal energy balance.

02 / FOLLOW IT THROUGH

A worked example

A constriction at fixed volume flow

  1. Set volume flow to one litre per second with first area four square centimetres.

  2. Set second area to one and compare speeds 2.5 and ten metres per second.

  3. Read second pressure about 353.13 kPa, below the initial four hundred, under the equal-height ideal assumptions.

OPTIONAL DEEPER DETAILGo deeper: inside the model

Inside this model

Fixed volume flow makes velocity inversely proportional to cross-section area. At equal height, pressure difference is half the water density times the difference in squared speeds.

03 / BEYOND THE EXPERIMENT

Where this idea is useful

A practical use

Distinguish a faster stream in a constriction from an increase in static pressure.

CHECK YOUR INTUITION

A common misconception

THE TEMPTING CONCLUSION

“Faster fluid must have higher static pressure everywhere.”

THE MORE USEFUL DISTINCTION

In this ideal horizontal streamline comparison, increased kinetic energy accompanies lower static pressure; added pumps or losses change the balance.

What this explanation leaves out

  • Steady incompressible inviscid flow without pumps is assumed. Geometry is schematic; turbulence, friction and energy losses are not predicted.
ONE MORE QUESTION

Does the pipe’s drawn height measure cross-section exactly?

No. The pipe is schematic; numerical areas and calculated velocities define the model, not the two-dimensional illustration.

TAKE THE IDEA WITH YOU

Are flow rate, velocity and pressure being treated as distinct quantities?

Associated thinkers

Associated withDaniel Bernoulli ↗

Associations marked provisional are awaiting source review.

Further reading

Explore the original research or the teaching reference behind this experiment.