MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS LECTURE 42: APRIL 25, 2005 - PowerPoint PPT Presentation

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MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS LECTURE 42: APRIL 25, 2005

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Title: MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS LECTURE 42: APRIL 25, 2005


1
MAE 3241 AERODYNAMICS AND FLIGHT
MECHANICSLECTURE 42 APRIL 25, 2005
  • Mechanical and Aerospace Engineering Department
  • Florida Institute of Technology
  • D. R. Kirk
  • Spring 2005

2
IMPLICATIONS AIRFOIL THICKNESS
Note thickness is relative to chord in all
cases Ex. NACA 0012 ? 12
  • Thick airfoils have a lower critical Mach number
    than thin airfoils
  • Desirable to have MCR as high as possible
  • Implication for design ? high speed wings usually
    design with thin airfoils
  • Supercritical airfoil is somewhat thicker

3
THICKNESS-TO-CHORD RATIO TRENDS
4
DRAG DIVERGENCE MACH NUMBER
  • Sharp increase in cd is combined effect of shock
    waves and flow separation
  • Freestream Mach number at which cd begins to
    increase rapidly is defined as Drag-Divergence
    Mach number
  • Modern airfoils may operate at point b

5
SWEPT WINGS
  • Explanation
  • Airfoil has same thickness but longer effective
    chord
  • Effective airfoil section is thinner
  • Making airfoil thinner increases critical Mach
    number
  • Sweeping wing usually reduces lift for subsonic
    flight

6
SWEPT WINGS
  • Recall MCR
  • If M8 gt MCR large increase in drag
  • Wing sees component of flow normal to leading
    edge
  • Can increase M8
  • By sweeping wings of subsonic aircraft, drag
    divergence is delayed to higher Mach numbers

7
WING SWEEP DISADVANTAGE
  • At M 0.6, severely reduced L/D
  • Benefit of this design is at M gt 1, to sweep
    wings inside Mach cone
  • Wing sweep beneficial in that it increases
    drag-divergences Mach number
  • Increasing wing sweep reduces the lift coefficient

8
TRANSONIC AREA RULE
  • Drag created related to change in cross-sectional
    area of vehicle from nose to tail
  • Shape itself is not as critical in creation of
    drag, but rate of change in shape
  • Wave drag related to 2nd derivative of volume
    distribution of vehicle

9
EXAMPLE YF-102A vs. F-102A
10
EXAMPLE YF-102A vs. F-102A
11
CURRENT EXAMPLES
  • No longer as relevant today more powerful
    engines
  • F-5 Fighter
  • Partial upper deck on 747 tapers off
    cross-sectional area of fuselage, smoothing
    transition in total cross-sectional area as wing
    starts adding in
  • Not as effective as true waisting but does
    yield some benefit.
  • Full double-decker does not glean this wave drag
    benefit (no different than any single-deck
    airliner with a truly constant cross-section
    through entire cabin area)

12
SUPERCRITICAL AIRFOILS
  • Supercritical airfoils designed to delay and
    reduce transonic drag rise, due to both strong
    normal shock and shock-induced boundary layer
    separation
  • Relative to conventional, supercritical airfoil
    has reduced amount of camber, increased leading
    edge radius, small surface curvature on suction
    side, and a concavity in rear part of pressure
    side

13
SUPERCRITICAL AIRFOILS
14
SUPERCRITICAL AIRFOILS
  • For given thickness, supercritical airfoil allows
    for higher cruise velocity
  • For given cruise velocity, airfoil thickness may
    be larger
  • Structural robustness, lighter weight, more
    volume for increased fuel capacity

757 wing
15
SMALL PERTURBATION VELOCITY POTENTIAL EQUATION
  • Equation is a linear PDE and easy to solve
  • Recall
  • Equation is no longer exact
  • Valid for small perturbations
  • Slender bodies
  • Small angles of attack
  • Subsonic and Supersonic Mach numbers
  • Keeping in mind these assumptions equation is
    good approximation
  • Subsonic 1 - M82 gt 0 (elliptic)
  • Supersonic 1 - M82 lt 0 (hyperbolic)

16
SUPERSONIC APPLICATION
  • Linearized small perturbation equation
  • Re-write for supersonic flow
  • Solution has functional relation
  • May be any function of (x - ly)
  • Perturbation potential is constant along lines of
    x ly constant

17
KEY RESULTS SUPERSONIC FLOWS
  • Linearized supersonic pressure coefficient
  • Expression for lift coefficient
  • Thin airfoil or arbitrary shape at small angles
    of attack
  • Expression for drag coefficient
  • Thin airfoil or arbitrary shape at small angles
    of attack

18
EXAMPLE FLAT PLATE
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