Добавил:
Опубликованный материал нарушает ваши авторские права? Сообщите нам.
Вуз: Предмет: Файл:
080 Principles of Flight - 2014.pdf
Скачиваний:
2437
Добавлен:
04.03.2019
Размер:
8.34 Mб
Скачать

Chapter

3

Basic Aerodynamic Theory

The Principle of Continuity . . . . . . . .

. . . .

. .

. .

. .

. .

. . . .

.

.

43

Bernoulli’s Theorem

 

 

 

 

 

 

 

 

44

Streamlines and the Streamtube

 

 

 

 

 

 

 

 

45

Summary

 

 

 

 

 

 

 

 

46

Questions . . . . . . . . . . . . . .

. . . .

. .

. .

. .

. .

. . . .

.

.

47

Answers . . . . . . . . . . . . . .

. . . . .

. .

. .

. .

. .

. . . .

.

 

.50

41

3

 

Basic AerodynamicTheory

 

 

 

 

Theory Aerodynamic Basic 3

42

Basic AerodynamicTheory

 

3

 

 

 

 

The Principle of Continuity

One of the fundamental laws of the universe is ENERGY and MASS can neither be created nor destroyed, only changed from one form to another. To demonstrate the effect this basic Principle of Continuity has on aerodynamic theory, it is instructive to consider a streamline flow of air through a tube which has a reduced cross-sectional area in the middle.

The air mass flow, or mass per unit time, through the tube will be the product of the crosssectional area (A), the airflow velocity (V) and the air density (ρ). Mass flow will remain a constant value at all points along the tube. The Equation of Continuity is:

A × V × ρ = Constant

Because air is a compressible fluid, any pressure change in the flow will affect the air density. However, at low subsonic speeds (< M 0.4) density changes will be insignificant and can be disregarded. The equation of continuity can now be simplified to: A × V = constant, or:

Velocity (V) =

Constant

Area (A)

Basic Aerodynamic Theory 3

Airflow

 

 

 

Cross-sectional

1 m3

½ m3

1 m3

Area (A)

Velocity (V)

52 m/s (100 kt)

104 m/s (200 kt)

52 m/s (100 kt)

Mass Flow

52 m3/s

52 m3/s

52 m3/s

(Constant)

 

 

 

Figure 3.1 The principle of continuity

Because the mass flow must remain constant, it can be seen from the equation of continuity that the reduction in the tube’s cross-sectional area results in an increase in velocity, and vice versa.

The equation of continuity enables the velocity changes of airflow around a given shape to be predicted mathematically, (< M 0.4).

43

3 Basic AerodynamicTheory

Bernoulli’s Theorem

“In the steady flow of an ideal fluid the sum of the pressure energy and the kinetic energy remains constant”.

3

Theory Aerodynamic Basic

Note: An ideal fluid is both incompressible and has no viscosity.

This statement can be expressed as: Pressure + Kinetic energy = Constant or:

p + 1/2 ρ V2 = Constant

Consider a mass of air: Static Pressure 101 325 N/m2, Density 1.225 kg/m3 and Velocity 52 m/s, its dynamic pressure will be: 1656 N/m2. [Q = ½ × 1.225 × 52 × 52]

Pressure (101 325 N/m2 ) + Kinetic energy (1656 N/m2 ) = Constant (102 981 N/m2 )

Figure 3.2 Bernoulli’s Theorem

Because the velocity of air at the throat has doubled, its dynamic pressure has risen by a value of four, and the static pressure has decreased. The significant point is that:

Static Pressure + Dynamic Pressure is a constant. This constant can be referred to either as:

TOTAL PRESSURE, STAGNATION PRESSURE or PITOT PRESSURE.

It can be seen that flow velocity is dependent on the shape of the object over which it flows. And from Bernoulli’s theorem, it is evident that an increase in velocity will cause a decrease in static pressure, and vice versa.

44

Соседние файлы в предмете [НЕСОРТИРОВАННОЕ]