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MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS

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Title: MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS


1
MAE 3241 AERODYNAMICS ANDFLIGHT MECHANICS
  • Design of Supersonic Airfoils
  • April 18, 2007
  • Mechanical and Aerospace Engineering Department
  • Florida Institute of Technology
  • D. R. Kirk

2
EXAMPLE OF SUPERSONIC AIRFOILS
http//odin.prohosting.com/evgenik1/wing.htm
3
SUPERSONIC AIRFOIL MODELS
  • Supersonic airfoil modeled as a flat plate
  • Combination of oblique shock waves and expansion
    fans acting at leading and trailing edges
  • R(p3-p2)c
  • L(p3-p2)c(cosa)
  • D(p3-p2)c(sina)
  • Supersonic airfoil modeled as double diamond
  • Combination of oblique shock waves and expansion
    fans acting at leading and trailing edge, and at
    turning corner
  • D(p2-p3)t

4
APPROXIMATE RELATIONS FOR LIFT AND DRAG
COEFFICIENTS
5
CASE 1 a0
Expansion
Shock waves
6
CASE 1 a0
7
CASE 2 a4
Aerodynamic Force Vector
Note large L/D5.57 at a4
8
CASE 3 a8
9
CASE 5 a20
At around a30, a detached shock begins to form
before bottom leading edge
10
CASE 6 a30
11
DESIGN OF ASYMMETRIC AIRFOILS
12
QUESTION 9.14
  • Consider a diamond-wedge airfoil such as shown in
    Figure 9.36, which a half angle e10. The
    airfoil is at an angle of attack a15 to a Mach
    3 freestream. Calculate the lift and wave-drag
    coefficients for the airfoil.

Compare with your solution
13
EXAMPLE MEASUREMENT OF AIRSPEED
  • Pitot tubes are used on aircraft as speedometers
    (point measurement)

Subsonic M lt 0.3
Subsonic M gt 0.3
Supersonic M gt 1
M lt 0.3 and M gt 0.3 Flows are qualitatively simil
ar but quantitatively different
M lt 1 and M gt 1 Flows are qualitatively and
quantitatively different
14
MEASUREMENT OF AIRSPEEDINCOMPRESSIBLE FLOW (M lt
0.3)
  • May apply Bernoulli Equation with relatively
    small error since compressibility effects may be
    neglected
  • To find velocity all that is needed is pressure
    sensed by Pitot tube (total or stagnation
    pressure) and static pressure
  • Comment What is value of r?
  • If r is measured in actual air around airplane
    (difficult to do)
  • V is called true airspeed, Vtrue
  • Practically easier to use value at standard
    seal-level conditions, rs
  • V is called equivalent airspeed, Ve

Static pressure
Dynamic pressure
Total pressure
Incompressible Flow
15
MEASUREMENT OF AIRSPEEDSUBSONIC COMRESSIBLE
FLOW (0.3 lt M lt 1.0)
  • If M gt 0.3, flow is compressible (density changes
    are important)
  • Need to introduce energy equation and isentropic
    relations

16
MEASUREMENT OF AIRSPEEDSUBSONIC COMRESSIBLE
FLOW (0.3 lt M lt 1.0)
  • How do we use these results to measure airspeed?
  • p0 and p1 give flight Mach number
  • Instrument called Mach meter
  • M1 V1/a1
  • V1 is actual flight speed
  • Actual flight speed using pressure difference
  • What are T1 and a1?
  • Again use sea-level conditions Ts, as, ps (a1
    (gRT)½ 340.3 m/s)
  • V is called Calibrated Velocity, Vcal

17
MEASUREMENT OF AIRSPEEDSUPERSONIC FLOW (M gt 1)
Rayleigh Pitot Tube Formula
18
EXAMPLE SUBSONIC AND SUPERSONIC FLIGHT
  • Flight at four different speeds, pitot measures
    p0 1.05, 1.2, 3 and 10 atm
  • What is flight speed if flying in 1 atm static
    pressure and Tambient 288 K (a 340 m/s)?
  • Determine which measurements are in subsonic or
    supersonic flow
  • p0/p 1.893 is boundary between subsonic and
    sonic flows
  • 1.05 atm ? p0/p 1.05 ? subsonic
  • Use compressible flow form, M 0.265, V 90 m/s
    200 MPH
  • Could use Bernoulli which will provide small
    error ( 1) and give V directly
  • Compressible form requires knowledge of speed of
    sound (temperature)
  • Apply Bernoulli safely? p0/p lt 1.065
  • 1.2 atm ? p0/p 1.2 ? subsonic
  • M 0.52, V 177 m/s 396 MPH
  • Use of compressible subsonic form justified
    (Bernoulli 3 error)
  • 3 atm ? p02/p1 3 ? supersonic
  • M1 1.39, V 473 m/s 1057 MPH (Bernoulli
    22 error)
  • 10 atm ? p02/p1 10 ? supersonic
  • M1 2.73, V 928 m/s 2076 MPH (MCO ? LAX in 1
    hour 30 minutes)
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