Fluid-Mechanics-Group-Assignment-Lukes-Part

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High-Speed Flight Assignment: How Bernoulli Effect changes from compressible air at subsonic speeds: When considering subsonic aerodynamics, lift is created by forces that are exerted on a body and the air (gas) which it is immersed in. With a speed of around ~300mph, the air is considered to be incompressible where, at a set altitude, its density is approximately the same whereas its pressure will vary. Based upon this assumption, water and air are acting the same and air can be classified as a fluid. Viscosity effects are said to be negligible when referring to subsonic theory and from this the result is the prevention of motion of a certain part of the fluid with respect to another. From this, it can be seen that air is classified as an ideal fluid, so it conforms to the principles of ideal fluid aerodynamics which include continuity, circulation and Bernoulli’s Theory. Of course, this is only theoretical, and the air is compressible and viscous in reality. When considering low speeds these effects are negligible but when speed increases the effects of compressibility become much more important and must be considered. It is very important to notice the effects of compressibility and also viscosity when the speed is higher and approaching the speed of sound. At these higher speeds, the density of the air surrounding the object is altered due to the compressibility effects present. When an accelerating airflow passes over the top surface of the wing this creates lift. Although the aircraft may only be at subsonic speed, this is not true for the accelerated air which reaches sonic speed. Having supersonic and subsonic airflows at the same time is possible when an aircraft is in flight. When the flow velocities achieve sonic speeds at certain locations on the aircraft (area of maximum camber of the wing), even more acceleration shows in the compressibility effects which take form in shock waves, buffeting, drag increases, stability along with trouble controlling. At speeds above this point, the subsonic flow principles can be disregarded. Bernoulli’s Equation for a Compressible Fluid: When at higher speeds, fluid density of gases will become constant and therefore can be disregarded. When increasing speed, air is undergoing compression which means the density is no longer constant and therefore will not be treated as such. When the flow is considered to have equal entropy, pressure and density have a relationship which can be described as: Where ‘y’ is the ratio of specific heats for the gas. The ratio for air is 1.4.
Figure: Aerodynamic Forces and The Boundary Layer: Aerodynamic forces are dependent on the viscosity of the gas although it is through a complex way. When an object moves through a gas, molecules from the gas stick to the surface of the object. When this occurs, the result is called a boundary layer, which is a layer of air near the object’s surface. As a result of this, the shape of the object is changed. The gas that flows past the boundary layer reacts with it as if it were a physical surface which is part of the object. It can get confusing when the boundary layer separates from the body which creates a new shape which is vastly different from the original shape of the object. Along with this, the interaction of the flow and the boundary layer are considered to be unsteady which means it changes with time. When considering the drag of an object, the boundary layer becomes very important. If trying to predict these conditions, it is vital to use a wind tunnel to test desired parameters along with a sophisticated computer evaluation to achieve a high level of accuracy in the results. Aerodynamic Forces and Compressibility: The compressibility of the gas is complexly dependent on the aerodynamic forces. When the object moves through/past the gas, the molecules of the gas shift around the object. When this occurs at low speeds (<200mph) the density for the fluid will be the same throughout. Whereas for high speeds, the object is compressed and takes away some of the energy to do so which then changes the density, from this the resulting force will change on the object. As the speed continues to increase the effects of compressibility become more evident and important. When speeds reach around and past the speed of sound (~330m/s), another effect becomes present in the form of shock waves, which will be noticed by the objects lift and drag. Once again when trying to test these results a wind tunnel along with an in-depth computer analysis will need to be carried out. The parameter of similarity for compressibility is known as the Mach number (M), which is the ratio of the velocity of the object (V) to the speed of sound (a). M = V / a
The Mach number is used as a parameter for scaling in a number of important equations which include shock waves and compressible flows. Velocity Distribution: An ideal fluid’s surface is known as a streamline as there are no boundary layers on the object. When the velocity is low, this means no energy is absorbed by the flow through compressibility and thus we can use Bernoulli’s equation to find its pressure magnitude and how its distributed along the streamline for a known velocity distribution. Once a boundary layer is involved, the edge of the boundary layer interacts with the external flow, along with the surface pressure being forced from the threshold of the boundary layer. This becomes more difficult when the boundary layer becomes separate from the object’s surface. Bernoulli’s Equation: Bernoulli’s equation is for non-viscous flows only. When considering this equation for a steady non-viscous compressible flow: Energy is conserved along any streamline of a flow -> (kinetic energy/mass) + (potential energy/mass) + (enthalpy/mass) P + 1 2 v 2 + +  = constant Or: 1 2 v 2 + gh + enthalpy per unit mass = constant
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References: Glenn, Valerie D. 2006. "NTRS: NASA Technical Reports Server200695ntrs: NASA Technical Reports Server. Washington, DC: National Aeronautics And Space Administration 1994 . Gratis Last Visited July 2005 URL: Http://Ntrs.Nasa.Gov/". Reference Reviews 20 (2): 40-41. doi:10.1108/09504120610647500. Richards, Louise M. 2008. "NASA Technical Reports Server (NTRS)2008364NASA Technical Reports Server (NTRS). Washington, DC: NASA Center For Aerospace Information Last Visited June 2008. Gratis URL: Http://Ntrs.Nasa.Gov/". Reference Reviews 22 (8): 40-41. doi:10.1108/09504120810914619. WOODWARD, F. A. 1968. "Analysis And Design Of Wing-Body Combinations At Subsonic And Supersonic Speeds.". Journal Of Aircraft 5 (6): 528-534. doi:10.2514/3.43979.

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