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# Fluid Dynamics

Let us consider a fluid, a drop of this fluid is falling and we can see that something  is dragging it backward making it not to fall, how far it can be stopped and to what extent it will flow? To know this we should know the concept of Fluid Mechanics. Fluid mechanics is a branch of physics which deals with the study of nature and properties of flow of fluid.

Fluid Dynamics is a branch of Fluid mechanics which stresses more on the fluid flow.

## What is Fluid Dynamics?

It is a part of fluid mechanics which signifies fluid flow. It includes:
1. Aerodynamics - It is concerned with the study of air in motion.
2. Hydrodynamics - It is concerned with the study of liquids in motion.
Applications :
• It can be used in traffic engineering (traffic treated as continuous liquid flow).
• To determine the flow rates of material like petroleum from pipes.
• To find and calculate the forces acting upon the air plane.
In fluid dynamics, fluid resistance refers to forces that oppose the relative motion of an object through a fluid, a liquid or gas. These drag forces act in an opposite direction to the flow of velocity. Drag forces depend upon velocity. For any solid object moving through a fluid, the drag is the component of the aerodynamic or hydrodynamic forces acting opposite to the direction of the movement. The component perpendicular to this direction is considered lift. Therefore, drag opposes the motion of the object.

## Fluid Dynamics Equations

Let the flow of the liquid be incompressible hence we will consider $\rho$ = constant,
$\frac{P}{\rho}$ + g z + $\frac{v^{2}}{2}$ = K
Or
$\frac{P}{\rho g}$ + z + $\frac{v^{2}}{2g}$ = K  Or
$\frac{P}{\rho g}$ + $\frac{v^{2}}{2g}$ + z = K ..........................(a)
where,
$\frac{P}{\rho g}$ = pressure energy per unit weight fluid or pressure head
$\frac{V^{2}}{2g}$ = kinetic energy per unit weight or kinetic head
z = potential energy per unit weight or potential head
P = pressure
$\rho$ = Density
K= constant
This is called Bernoulli's Equation.

Here, the flow of fluid particle along a stream line in the S direction is considered. The resultant or net force in the S direction is equated to the mass of fluid particle and its acceleration, now the flow of the compressible fluid is constant:
$\frac{dP}{\rho}$ + V dV + g dZ = 0
$\int$ ($\frac{dP}{\rho}$ + V dV + g dZ) = K
or
$\int$ $\frac{dP}{\rho}$ + $\frac{V^{2}}{2}$ + g Z = K
The Bernoulli equation is different for adiabatic as well as isothermal processes.
Here,
Z = elevation point and
$\rho$ = Density of fluid

We can write the equation in other form:
q +  P = Po ................................(b)
Here,
q = dynamic pressure
Po = total pressure
P = Static pressure

## Fluid Flow

The Science of fluids in motion is called Fluid Flow. The fluids can be liquids and gases but not solid. Fluid flow basically signifies the flow of a fluid under various situations like through a pipe, hole etc. It talks about properties of incompressible as well as compressible fluid when under flow. We will also study about the continuity equation which is different for both types of fluid.
For incompressible it is: A1V1 = A2V2
For compressible fluid it is: p1A1V1 = p2A2V2
where, A1 and A2 are Areas
p1 and p2 are pressures
V1 and V2 are Volumes

Fluid Flow is categorized as,
(i) Streamline or laminar flow
(ii) Turbulent flow
Pascal's law : It states that a change in pressure at any point in an enclosed fluid at rest is transmitted undiminished to all points in the fluid. i.e. the pressure applied in a confirmed incompressible fluid will be transmitted equally in all directions in the fluid.

## Archimedes Principle

The Archimedes Principle states that:
When an object floats into the fluid then it displaces its own weight of fluid. Now it should be noted that gas is also a kind of fluid.
Hence, the law becomes:
When an object or body is immersed in a liquid fully or partially then it  experiences an upward force which is in correspondence with the amount of water or fluid displaced.
We can also say that,
Buoyancy = the weight of the fluid displaced...............(a)

For example: The hot air balloon rises in the air as the density of the warmer air  inside the balloon is lesser than the cool air outside the balloon. There is buoyant force acting on the system and so, the balloon as well as the basket displaces a fluid that is heavier than both of them.
This is the reason balloons tend to fly better in the morning as the surrounding air is cool.

The apparent weight of the object = The original weight – the buoyant force exerted..................(b)

## Density

Density is described as the mass of a substance per unit volume. It was discovered by Archimedes. Mathematically, Density is defined as:
Density = $\frac{Mass}{Volume}$It is represented by a symbol called $\rho$.
The Units are kg / m3.
For example: Wood floats on water because it has a lower density than water.

## Buoyancy

The Upward force experienced by the fluid on the body or the object when it is inserted or immersed in the fluid is called Buoyancy.
The point where the force of Buoyancy is exerted or the point on the body where the force acts is called the Center of Buoyancy

Why do you think the crown in water feels lighter than it actually is? When we immerse the body in a fluid then an upward force is experienced by the body. This force is exerted by the fluid on the body which makes it to rise up and is called the Force of Buoyancy. The magnitude of this force is exactly equal to the amount or weight of the liquid displaced.

It should be noted that the force of buoyancy is a vertical force and hence the center of buoyancy is the point located on the center of the gravity of the liquid that is being actually displaced by the object immersed.

## Bernoulli's Principle

gh + $\frac{1}{2} v^{2}$ + $\frac{p}{\delta}$ = constant
Here, $\frac{p}{\delta}$, i.e., the ratio of pressure to density is the pressure energy per unit mass of the moving liquid. According to Bernoulli's principle, if we add all the energy components of the flowing fluid along the streamline then we would get a constant value for it throughout the flow of line. Even the sum of the potential and kinetic energy follows a constant value.