Bernoulli equation, or the incompressible steady flow energy equation, is considered one of the most well-known equations in physics ( fluid mechanics) and it explains the conservation of mechanical work-energy. The equation was published in 1738 by Daniel Bernoulli (a Swiss physicist) to help us understand fluid flow.

Daniel Bernoulli was born on February 8th, 1700, in the Netherlands. He studied mathematics and medicine under the guidance of his father Johann Bernoulli.

In this article, we will discuss Bernoulli equation, principle, derivation, application and more.

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Table of Contents

## **Bernoulli Equation**

P is the static pressure (the pressure of the fluid)

ρ is the density

V is the velocity

G is the gravitational acceleration

H is the elevation of the fluid

Bernoulli’s theorem describes the relation between velocity, pressure, and elevation of a flowing fluid in a streamline.

It states that the dynamic pressure plus the static pressure in the flow, one half of the density (r) times the velocity (V) squared, is equal to a constant throughout the flow. The constant is called the total pressure of the flow (pt).

Or simply, the Bernoulli equation states that the sum of the potential, kinetic, and flow energies of a fluid is constant in a streamline in steady flow.

Note:

The streamline in steady flow is the path traced by a single particle within the fluid.

The following figure shows the streamline in steady flow:

To apply Bernoulli’s equation:

- The flow must be steady (Velocity, density, and pressure must not change at any point in the streamline).
- The flow must be incompressible: even when the pressure varies, the density must remain constant along the streamline.
- Friction by viscous forces must be negligible or minimal.

Note:

Incompressible flows are gasses and gasses with a low Mach number and constant fluid density, regardless of the pressure flow. By using incompressible flow, we will have the simplest form of Bernoulli’s equation

**Bernoulli’s Principle**

Bernoulli’s principle states that an increase in the velocity (the speed of a fluid) occurs simultaneously and must be accompanied by a decrease in the potential energy of the fluid (or the static pressure).

Bernoulli’s principle can be derived from the conservation of energy principle. In case of steady flow, the sum of energy forms in a fluid will remain the same at all points of that streamline. While all the energy remains constant, an increase in the fluid velocity will imply that there is an increase in the kinetic energy or dynamic pressure. This happens with a decrease in the potential energy (the static pressure and internal energy).

**Bernoulli’s Principle Formula**

Bernoulli’s equation formula is considered a relation between pressure, potential energy, and kinetic energy of a fluid.

The formula given is as follows:

The Bernoulli equation can be considered to be the conservation of energy principle for the flowing fluids. Bernoulli effect is the lowering of fluid pressure in cases where the velocity is increased. In the case of high velocity flow through the constriction, the kinetic energy must increase at the expense of pressure energy.

**Limitations on the Use of Bernoulli Equation**

The Bernoulli equation is applicable to steady flow as we explained before, but in some cases we can’t use the Bernoulli equation.

The Bernoulli theorem is not applicable in a flow section like machines (e.g., fan or turbine or pump), because these machines can damage the streamlines and make energy interactions with the fluid. So in these cases, the energy equation should be used instead of Bernoulli equation.

The equation also should not be used for significant temperature change flow sections like cooling or heating sections, because the gas density is inversely proportional to the temperature.

Every flow involves some friction and if the frictional effects are not be negligible, the Bernoulli theorem is not applicable in this case.

So, the Bernoulli equation should not be used in the flow of:

- Sudden expansion
- Heating section
- Valve
- Fan
- Narrow long tube

**Bernoulli Equation Derivation**

We can drive Bernoulli differential equation as follows:

We will consider that we have a pipe with a varying height and diameter through which an incompressible fluid is flowing. The relationship between the areas of cross-sections A, pressure p the speed of the flow v, and the height h at two different points 1 and 2 is described in the following figure:

**Assumptions:**

- The incompressible fluid density remains constant at both points.
- The fluid energy is conserved because there are no viscous forces in the fluid.

So, the work done on the fluid is given as:

dW = F1dx1 – F2dx2

dW = p1A1dx1 – p2A2dx2

dW = p1dv – p2dv = (p1 – p2)dv

We know that the work done on the fluid was due to the conservation of change in both the kinetic energy and gravitational potential energy

The change in kinetic energy of the fluid is given as:

The change in potential energy is given as:

dU = m2gy2 – m1gy1 = ρdvg(y2 – y1)

Then, the energy equation is given as:

dW = dK + dU

And finally by rearranging the above equation, we get

**For more understanding, watch the following video about Bernoulli equation derivation**

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**Bernoulli Equation Applications**

Bernoulli’s equation has many applications. For example, we can use it to explain how planes generate lift, to calculate the velocity of fluid flow, or why ships have to run away from each other as they pass, and other applications that we find in our daily lives. We will go over in detail some of the most popular of these applications.

**Bernoulli equation application in fluid mechanics**

The Bernoulli equation is applied to all incompressible fluid flow problems. The Bernoulli equation can be applied to devices such as the orifice meter, Venturi meter, and Pitot tube and its applications for measuring flow in open channels and inside tubes.

Venturi meter is a device that is based on Bernoulli’s principle and used to determine the rate of flow through a pipe. It works by measuring the pressure drop across a section near the pipe. For an incompressible fluid, reducing the diameter will increase the fluid flow velocity.

Note: Bernoulli’s principle states that there must be a pressure drop in the region of the reduced diameter. This phenomenon is known as the venturi effect.

**Venturi meter**

**Application of Bernoulli’s equation in pumps**

As we mentioned before,the speed of a fluid flow can be measured by devices like Venturi meter, which is used to reduce the diameter of the flow and placed into a pipeline.

The maximum possible discharge rate for a tank with an opening or a spout at the base can be calculated directly by Bernoulli’s equation, and it has been found to be proportional to the square root of the height of the liquid in the tank (this is Torricelli’s law) and this shows that Torricelli’s law is compatible with Bernoulli’s principle. Viscosity reduces the rate of discharge.

**Aeroplanes**

How aircraft wings generate lift can be explained by Bernoulli’s equation for fluids. In the case of flight, the fluid flowing above the wing of the aircraft moves faster than the flowing under the wing, and according to Bernoulli’s principle this causes the creation of a region of low pressure above the surface of the air and a region of high pressure under the plane and this pressure difference is what generates altitude.

That is, we can explain the reason for the shape of the wings and their upward curvature (according to Bernoulli’s theory) that the air passes at a higher speed on the upper surface than the lower one. The difference in air velocity is calculated using Bernoulli’s principle of difference in pressure.

**Pressure detection**

In some cases of fluid flows, we know the velocities at two points of the streamline and pressure at only one point. The unknown is the pressure at the other point of the fluid.

So in this case (if the Bernoulli equation applies to it ) we can use Bernoulli’s Equation to find the unknown pressure.

**Velocity detection**

In cases where the elevation and pressure at two points of the streamline are known and velocity at one point is also known, and we want to find the unknown velocity, Bernoulli’s Equation is applied to calculate and find the required velocity.

**For example: the flow through a siphon**

In this case, we need to find the velocity with which the fluid leaves the siphon. By applying Bernoulli’s Equation between the reservoir surface and the siphon exit point where the fluid leaves the tube, pressure at both points is the same and equal to the atmospheric pressure, and the velocity at the reservoir is negligible because the reservoir is large. We can calculate the velocity at the exit point by using the values of elevation at the two points.

**Application of Bernoulli’s equation in medicine**

In echocardiography, Bernoulli’s principle can be applied when interpreting blood flow to describe a localized pressure decrease produced by high flow rate near blockages.

For clinical medicine, the equation is used for an easy estimation of pressure gradients from velocity.

Bernoulli’s equation can also be used in the venturi mask.

The venturi mask is a medical oxygen device that delivers oxygen concentration to patients on controlled oxygen therapy. The mask has a tube that is connected to a nozzle which connects to a supply of pure oxygen. The tube that is directly connected to the mask has a small window which allows room air to flow into the mask.

The venturi mask can control the amount of oxygen that flows in, along with pure oxygen delivered from its connected nozzle.

**Venturi masks** use the Bernoulli principle, As oxygen flows into the tube, it creates a decrease in pressure due to oxygen passing through a narrow opening of the tube. The air is allowed to flow into the mask by the drop of pressure, mixing with the pure oxygen from the nozzle, which is the consequence of Bernoulli’s principle.

**Other Applications of Bernoulli’s Principle**

- Bernoulli’s theory is used to study the unstable potential flow used in the theory of ocean surface waves and acoustics.

- When we stand at a railway station and a train comes in, we tend to fall towards the train. We can explain this using Bernoulli’s principle. As the train passes, the speed of the air between us and the train increases. Hence, from the equation, we can say that the pressure is decreasing. So the pressure from the back pushes us towards the train and that depends on the Bernoulli effect.

- The Bernoulli equation also explains how a Bunsen burner works. When the gas valve is opened, the gas flows into the barrel at a high velocity. According to Bernoulli’s theory, this high velocity creates a low pressure area in the barrel (which draws air through the regulator) allowing the gas to burn more efficiently.

- Many flow meters are based on Bernoulli’s principle to determine the velocity of a flowing fluid. The most famous of these devices is the Pitot-Static Tube, which is used in aircraft to measure flight speed.

- Bernoulli’s principle also applies to swinging a cricket ball. During the match, players constantly polish one side of the ball. After some time, one side is completely rough and the other is still smooth. Hence, when the ball is thrown in the air, the velocity on one side of the ball is faster than the other, due to this difference in smoothness. And this leads to a difference in pressure between the two sides. This causes the ball to spin (“swing”) as it travels through the air.

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