Introduction to UAV Systems. Mohammad H. Sadraey. Читать онлайн. Newlib. NEWLIB.NET

Автор: Mohammad H. Sadraey
Издательство: John Wiley & Sons Limited
Серия:
Жанр произведения: Техническая литература
Год издания: 0
isbn: 9781119802624
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of propulsion (Chapter 6) commonly used by UAVs are explored, including an introduction to the subject of rotary wing (e.g., quadcopter) and ducted fan concepts. Finally, some structural and load (Chapter 7) topics of importance to UAV engineers are described.

      3.1 Overview

      Aerodynamics is the science that involves the study of the behavior (i.e., dynamics) of air when confronting a moving object (e.g., air vehicle). The UAV has a number of components that are characterized by their aerodynamic outputs (e.g., lift), two of which are wing and tail. A wing/tail is considered as a lifting surface in which the lift is produced due to the pressure difference between lower and upper surfaces. In contrast, surfaces such as aileron, rudder, and elevator are referred to as the control surfaces. Lifting surfaces are generally fixed while control surfaces are always moving up/down or left/right. Both lifting and control surfaces are functions of their aerodynamic features.

      The primary aerodynamic function of the wing and tail is to generate sufficient lift force or simply lift (L). However, they have two other undesirable products, namely drag (D) and nose‐down pitching moment (M). The fuselage is not fundamentally considered as an aerodynamic component based on its function. However, fuselage has a considerable role in creating drag, while it generates a little lift.

      In this chapter, aerodynamic forces (mainly lift and drag), airfoil, pressure distribution, friction drag, induced drag, drag polar, air vehicle drag, boundary layer, and aerodynamic efficiency will be briefly covered.

Schematic illustration of forces on an air vehicle during a level flight. Schematic illustration of aerodynamic lift, drag, and pitching moment.

      The aerodynamic forces of lift and drag [8] are functions of the following factors: (1) aircraft configuration, aircraft/wing angle of attack (α), (3) aircraft geometry, (4) airspeed (V), (5) air density (ρ), (6) Reynolds number of the flow, and (7) air viscosity:

      (3.1)upper L equals one half rho upper V squared upper S upper C Subscript normal upper L

      (3.2)upper D equals one half rho upper V squared upper S upper C Subscript normal upper D

      where ρ is air density, V is velocity, S is the wing planform area, and CL and CD are the lift and drag coefficients respectively. The calculations of lift and drag coefficients will be presented in the coming sections.

      The lift force or simply lift is always defined as the component of the aerodynamic force perpendicular to the relative wind. The drag is always defined as the component of the aerodynamic force parallel to the relative wind (V). In other words, lift is always perpendicular and drag is always parallel to the relative wind. Figure 3.2 shows an airfoil section and the directions of lift and drag.

      In reality, the aerodynamic force is located at the center of pressure (cp), which is moving with the variations of angle of attack (α). However, the aerodynamic center (ac) which is frequently selected to be the center of lift, is located nearly at the quarter chord (i.e., 1/4 of C). The pitching moment is the bi‐product of moving the location of aerodynamic force from cp to ac. The moment can be taken with respect to any point, but traditionally is taken about a point 25% rearward of the wing leading edge, known as the quarter chord. The aerodynamic center has a desired property – the variation of moment coefficient with respect to the angle of attack is zero (i.e., moment coefficient remains constant).

      It is customary to compare the speed of an air vehicle (V) with the speed of sound (a). The Mach number is defined as the ratio of airspeed over the speed of sound:

      (3.3)upper M equals StartFraction upper V Over a EndFraction

      The speed of sound at the sea level standard condition is 340 m/s. M is used to define four different flight regimes for airspeed: (1) subsonic, (2) transonic, (3) supersonic, and (4) hypersonic.

      When the flight speed is less than the speed of sound – where M < 1 – it is defined as subsonic speed. When 0.8 ≤ M ≤ 1.2, the flight regime is loosely defined as transonic. If the flight speed is less than the speed of sound, but M is sufficiently near 1, the airflow expansion over the top surfaces of the wing/tail/fuselage may result in locally supersonic regions. A flowfield where M > 1 everywhere is defined as supersonic. At supersonic speeds, a shock wave (e.g., normal, oblique, and bow) is created by nature to adjust the flow properties (e.g., air pressure and temperature).

      The flow regime for M > 5 is given a special label, hypersonic flow. For values of M > 5, the shock wave is very close to the surface, and the flowfield between the shock and the body (the shock layer) becomes very hot indeed, hot enough to dissociate or even ionize the gas. The aerodynamic characteristics of an air vehicle is strongly a function of Mach number, some of which will be discussed in this chapter.

      If