# Basic Aerodynamics Theory

Understanding how an aeroplane derives lift with the Bernoulli's equation, and looking at the forces acting on an aeroplane in flight.

## Introduction

### Key Facts

*Definitions***Law of Conservation of Energy**Energy can neither be created, nor destroyed. It can only be said to change its state from one to another. As such, the total energy in any given system is always a constant.

**Bernoullis principle**

For a perfect incompressible liquid, flowing in a continuous stream, the total energy of a particle remains the same, while the particle moves from one point to another.

**Kutta condition**

A body with a sharp trailing edge which is moving through a fluid will create about itself a circulation of sufficient strength to hold the rear stagnation point at the trailing edge.

**Lift**

It is the component of force acting upwards and perpendicular to the line of flight, in a steady, undisturbed stream of air. It is important to note that 'upwards' implies to the roof of the aircraft in all attitudes of flight, i.e. Upright, Banked (as during a turn), and Inverted.

Aero-dynamics is the study of the dynamics associated with the motions of air over a moving object. When an aircraft accelerates down the runway to take off, it produces a relative motion between the air and the aircrafts wings. It is this rush of airflow over and below the wings, created by the aircrafts forward motion, which produces lift and consequently makes all forms of powered flight possible.
The contours of the upper and lower surfaces of the wing contribute largely to the pressure differences that occur between the two surfaces. The resulting pressure leads to a net force that provides 'Lift' to the wing.
In this section, we use the Bernoulli's and Euler's equations to understand how an aeroplane derives lift. We also look at the four principle forces acting on an aircraft in flight, at ALL times.

### Bernoulli's Equation

- As with all applications of the Bernoulli's principle, we shall assume that the flow of air around the aerofoil is:
- Steady,
- Incompressible, and
- Frictionless.

- and is the Pressure of the fluid at Point and respectively
- and is the Velocity of the fluid at Point and respectively
- and is the vertcal elevation at Point and respectively
- is the Density of the fluid
- is the acceleration due to gravity

Using Bernoulli's equation from (1), equating the values of pressure and velocity at this point () with those of ambient air, we get: From Eq (2) and (3) we have: According to the Kutta condition of circulation, the airflow over the upper surface of the aerofoil is faster than that below the underside of the aerofoil.

i.e. Therefore, to satisfy the condition given in Eq(4),**The net result is an upward acting force which is termed as 'Lift'.**

## Forces Acting In Flight

In the following diagram, we see four forces acting on an aircraft at all times. When an aircraft is in level flight, all the four fources are balanced and the aircraft can be said to be in a state of Equilibrium.Lift() = Weight(), and

Thrust() = Drag()

In such state the aircraft will be travelling at a steady height, at a uniform velocity, and fixed heading.

### Climbing And Descending

- The following discussion explains the relationship between these four forces when an aircraft is in the phase of gaining altitude (climbing), and when the aircraft descends.
In the above diagram, consider the angle of climb to be .
Resolving the vectors about , we get:
- component directly opposing Thrust ; and,
- component directly opposing Lift .

- (It is important to note the definition of Lift in this context)

: As we shall see in a later section, the ratio of L and D also has a significant effect on the Range and the Endurance(in other words the Performance) of the aircraft.*Note**Note regarding Numericals*In working out numericals associated with the Forces in Flight, it is important to note that the vectors (, , , ) are merely representative, and do not indicate their actual position. This is further explained in the diagram below. In low wing aircrafts, the vector is often located ahead of the vector; providing a couple with a nose-down pitching moment. Similarly, and directly opposing this (-) couple, the vector is located below the vector; providing a couple with a nose-up pitching moment.*Note: In the event of loss of power (),the nose-down pitching moment takes precedence, allowing the aircraft to enter into a glide. If a nose-up pitching moment was provided in such an event, the aircraft would inevitably stall and descend uncontrollably earthward. Thus the need for Weight and Balance of an aircraft, and the need to ensure that the C of G is within limits. This will be further analysed in future pages.*In addition,the forces acting on the Mainplane (Wings) are balanced by similar forces acting on the Tailplane (Stabilizer). All such numericals can be solved withe reference to the law of moments.

Example:

##### Example - Level Flight - With No Tail Plane Load

Problem

A seaplane of mass 20000 Kg. is flying in Straight and Level Flight. The thrust vector is located 1.2m ABOVE the drag vector. If the Lift/Drag ratio is 5:1, calculate the position of the lift vector. Consider the forces on the tail plane to be absent or negligable. Assume

Workings

By resolving the vectors it can be seen that in this case the Thrust and drag vectors produce a nose-down pitching moment. To oppose this, the Lift and Weight vectors will produce a nose-up pitching moment, i.e. Lift vector ahead of weight.
Let be the moment arm between and
In st. and level flight we know,
= = 20000g kN
ratio = 5:1
Therefore, = 4000g kN =
Resolving the moments we get,

Solution

= 0.24m
The Lift vector is positioned 0.24m ahead of the Weight vector.