Bernoulli's theorem describes the distribution of pressure, velocity and altitude in an ideal fluid flow. At the heart of this theorem: the total energy along a flow line remains constant. This fundamental principle is used in aerodynamics and in various fluid systems.
At the heart of the mysteries of fluid mechanics lies Bernoulli's theorem. Simplifying the relationship between pressure and velocity in liquids and gases, this principle governs the operation of a wide variety of applications, from the aeronautical industry to fountains.
This article details its origins, key concepts and practical implications.
Imagine a peaceful stream suddenly accelerating into a roaring waterfall. This change in the water's behavior is no mere whim of nature, but a manifestation of Bernoulli's principle.
According to this principle, in a fluid flow, pressure is inversely proportional to velocity: where the flow accelerates, pressure decreases, and vice versa.
It's a fluid, harmonious ballet, where each particle of water dances according to the laws of fluid mechanics, alternating between kinetic energy and dynamic pressure to maintain a delicate, constant balance.
This phenomenon is ubiquitous, and applies to rivers as much as to the air currents that envelop the wings of airplanes, enabling them to soar into the skies.
At the heart of this story is one man, Daniel Bernoulli, whose brilliant mind illuminated the mysteries of fluid motion. A Swiss physician, physicist and mathematician, Bernoulli was a polymath who transcended disciplines to lay the foundations of fluid dynamics.
Born into a family of illustrious scholars, he inherited an ardent passion for science and pursued a diverse academic career, imbuing himself with the wisdom of his father Jean and his uncle Jacques. His teachings at the University of Basel covered astronomy, medicine and philosophy, reflecting his universal spirit. It was in his treatise 'Hydrodynamica', published in 1738, that Bernoulli revealed to the world the principle that would bear his name, and which was to become a pillar of fluid mechanics and aerodynamics.
Bernoulli's equation is the mathematical embodiment of his principle, a formula that synthesizes the relationship between pressure, velocity and height of a fluid moving along a streamline. This equation, which derives from the conservation of energy in a permanent, incompressible flow, is a cornerstone of fluid mechanics.
It illustrates the fact that, despite the transformations and movements of fluid particles, their total energy remains constant, a testament to the universal law of conservation of energy.
In detail, each term in Bernoulli's equation is of crucial importance and represents an aspect of the system's total energy. Pressure, for example, is simply the expression of the force the fluid exerts on the surfaces with which it interacts.
The term density, although not explicitly defined in our sources, represents the quantity of matter contained in a unit volume and is of vital importance in calculating the kinetic energy of the fluid, which is directly related to its velocity in m s.
Finally, altitude and gravity, which have a direct impact on potential energy, complete the picture by contributing to the sum of energies within the equation.
Bernoulli's equation is useful in concrete applications, such as the Venturi tube, where it demonstrates its effectiveness by revealing how pressure varies as a function of tube cross-section.
In this context, the fluid accelerates as it passes through an area of reduced cross-section, leading to a decrease in pressure, then slows down and sees its pressure increase as the cross-section widens, an eloquent demonstration of Bernoulli's conservation of quantity throughout the fluid.
This same logic explains why, in a fountain, water gushes vigorously upwards from a horizontal buried section, invariably following the principles of Bernoulli's equation.
Bernoulli's theorem, far from being an academic curiosity, has proved an invaluable tool in many practical applications. The design of aircraft wings, for example, relies heavily on this principle: the shape of the wing modifies the speed of the air and, consequently, the pressure, creating the lift necessary for flight.
This is also the case for measuring instruments such as the Pitot tube, used to calculate air speed in relation to an aircraft by studying different pressures.
There are many industrial applications, such as volume flow measurements of liquids, gases, biogas and steam using depressurizers (Pitot tube, orifice plate, venturi tube, nozzle, integrated orifice) with pressure transmitter differential. When velocity is zero in Bernoulli's theorem equation, then the law of hydrostatics applies.
Hydrostatic level measurements are used to monitor the volume values of raw material liquids in tanks using pressure transmitter hydrostatic.
Even the Magnus effect, that amazing phenomenon where a rotating cylinder generates a lateral force by creating a pressure difference, finds its explanation in Bernoulli's theorem.
But the Bernoulli effect is not limited to airplanes and Pitot tubes. It manifests itself spectacularly in our everyday lives. When we blow between two cans, for example, we observe the Venturi effect: the increase in air velocity reduces the pressure between them, bringing them closer together.
This fascinating interplay between fluid velocity and pressure can be playfully demonstrated by manipulating air in a narrowed neck or with sheets of paper.
The relationship between fluid velocity and pressure is a fundamental concept in modern engineering.
In aerodynamics, for example, it is essential for understanding the lift of aircraft wings and the design of more efficient vehicles. Bernoulli's theorem also plays a role in the development of technologies such as..:
These examples illustrate the importance of the relationship between fluid velocity and pressure in many areas of engineering.
But fluid mechanics doesn't stop at Bernoulli's principle. It encompasses more complex concepts such as viscosity, which measures a fluid's resistance to flow and depends on temperature, among other factors.
The flows themselves can be classified as laminar or turbulent, a distinction determined by the Reynolds number, which takes into account fluid velocity and viscosity.
However, Bernoulli's theorem is not without its limitations. In the real world, fluid flows are often affected by viscous effects, pressure losses or heat transfers that are not taken into account by the theorem in its simplest form.
Furthermore, in systems where pumps, turbines or valves are present, adjustments to Bernoulli's equation are necessary to consider the power added to or subtracted from the fluid.
At the end of our exploration, we've traversed the fascinating spectrum of Bernoulli's theorem, from its historical origins to its modern implications in fluid mechanics and beyond. We demystified its equation, explored its practical applications and even revealed its limits. This journey revealed how much our world is shaped by the laws of fluid dynamics and how, even without being aware of it, we experience the effects of Daniel Bernoulli's brilliant discovery on a daily basis.
Bernoulli's principle establishes a relationship between the velocity and pressure of a moving fluid, indicating that pressure decreases where fluid velocity increases, and vice versa.
Bernoulli's equation is used to design airplane wings in order to generate the lift required for flight by modifying the speed of the air around the wings, thus influencing the pressure.
Yes, Bernoulli's equation applies to both liquids and gases, provided the fluid is incompressible and the flow is permanent and frictionless.
Bernoulli's theorem has its limits in cases involving high pressure drops, viscous effects, heat transfer or non-incompressible flows.
The Magnus effect is a phenomenon where a rotating object creates a pressure difference on its sides in a fluid, resulting in a lateral force. This is explained by Bernoulli's principle, as rotation affects the speed of the fluid and therefore the pressure around the object.
