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Aerodynamics Chapter 3 Aerodynamics of Flight
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Figure 3-1. Balance of forces and moments.
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Figure 3-2. Indicated airspeed varies inversely with angle of attack.
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Figure 3-3. At a constant angle of attack, a lighter airplane must fly slower.
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Figure 3-4. Same power–lighter airplane has a lower angle of attack and flies faster.
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Figure 3-5. The thrust-required or drag curve.
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Figure 3-6. Both low speed and high speed require high thrust.
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Figure 3-7. The power-required curve.
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Figure 3-8. Maximum level-flight speed.
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Figure 3-9. Graph of drag versus TAS.
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Figure 3-10. Graph of power versus TAS.
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Figure 3-11. Speed stability.
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Figure 3-11. Same IAS (and lift) at a higher altitude means higher TAS.
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Figure 3-11. A zoom and a steady climb.
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Figure 3-12. The four forces in equilibrium in a steady climb.
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Figure Maximum angle climb, maximum rate climb, cruise climb; use the one that suits the situation.
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Figure 3-14. Fly at the correct climb speed for best performance.
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Figure 3-15. Climb performance decreases with altitude.
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Figure 3-16. A typical climb performance table.
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Figure 3-17. Wind affects the flight path achieved over the ground.
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Figure 3-20. “Thrust required” and “thrust available” versus TAS.
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Figure 3-21. Climb gradient may be less with flaps extended.
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Figure 3-22. “Power required” and “power available” versus TAS.
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Figure 3-23. Flying the incorrect airspeed reduces excess thrust and angle of climb.
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Figure 3-24. Flying the incorrect airspeed reduces excess power and rate of climb.
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Figure 3-25. In a glide descent, a component of weight counteracts the drag.
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Figure 3-26. A smaller L/D ratio (increased drag) results in a steeper glide.
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Figure 3-27. Angle of attack versus L/D ratio.
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Figure 3-28. The flattest glide is achieved at the maximum L/D ratio.
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Figure 3-29. Steeper glide angle with flaps extended.
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Figure The best glide angle is the same at all weights (maximum L/D) but the airspeed must be lower at lower weights.
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Figure 3-31. More ground is covered gliding with a tailwind and less with a headwind.
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Figure 3-32. “Air distance/altitude” is the same ratio as “lift/drag.”
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Figure By banking, the tilted lift force has a horizontal component which provides the centripetal force.
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Figure 3-34. The centripetal force pulls a body into a turn.
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Figure 3-35. The steeper the bank, the greater the lift force required from the wings.
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Figure 3-36. The steeper the bank angle, the greater the g-forces.
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Figure 3-37. Load factor versus bank angle.
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Figure 3-38. A steep level turn requires increased lift.
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Figure 3-40. Percentage increase in stall speed versus bank angle.
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Figure 3-41. A standard-rate turn requires a steeper bank angle at a higher airspeed.
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Figure 3-42. Turning performance is increased at low airspeeds.
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Figure 3-43. Constant-radius turn.
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Figure 3-44. A steeper bank angle at constant speed increases turn performance.
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Figure 3-45. An airfoil reaches its maximum lifting ability at the critical angle of attack.
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Figure 3-46. Turbulent flow over the horizontal stabilizer.
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Figure The stall occurs at the same stall angle in all phases of flight, but not necessarily at the same speed.
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Figure 3-48. Stall speed increases with load factor.
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Figure 3-49. Relationship between stall speed, load factor and bank angle.
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Figure 3-50. Stall speed is a function of weight.
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Figure 3-51. Slipstream can lower stall speed.
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Figure 3-52. Examples of stall speeds in different situations.
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Figure 3-53. Built-in washout causes the wingtip to stall later than the root.
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Figure 3-54. The boundary layer over a flat surface.
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Figure 3-55. The boundary layer over the wing’s upper surface.
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Figure 3-56. The flight path in a spin.
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Figure 3-57. The airplane in a stable spin to the left.
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Figure Close to the stall, reduced lift and increased drag on a dropping wing cause autorotation.
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Figure 3-59. Lift and drag effects on a dropping wing.
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