Aerodynamic Forces (Lift) Flashcards

1
Q

Define the following (of a wing):

  • Chord line
  • Mean camber line
  • Camber
  • Thickness
  • Leading edge radius
A
  • Line joining leading and trailing edge
  • Line equidistant from upper/lower surface of the wing
  • Thickness between MCL & chord line
  • Distance between upper and lower surface
  • Radius of the curvature of the leading edge
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2
Q

Describe the meaning of the 1st, 2nd & 3rd/4th digits in the NACA system

A

1st digit: Max camber as a percentage of the chord
2nd digit: Location of max camber from the LE as a 10th percentage of the chord
3rd/4th digit: Max thickness of the aerofoil as a percentage of the chord

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3
Q

What is the trend for the NACA system for symmetrical aerofoils?

A

The first two digits are 0 as the MCL=chord so you are unable to determine the location of the max thickness

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4
Q

Draw the pressure envelopes of -4* AoA through to 20* AoA & the forces of an aerofoil

A

Refer to notes for diagrams

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5
Q

What is the pressure coefficient equal to (Cp)?

What is Cp?

A
Cp= (P-Pfs)/q
P: local pressure
PNS: freestream static pressure
Q: dynamic pressure
A dimensionless quantity measuring ratio of local pressure and freestream pressure to dynamic pressure
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6
Q

What is the line of zero lift?

A

The edgewise straight line through the aerofoil, parallel to the airflow, when the aerofoil points downwards and produces no lift.
Does NOT mean no moment.
Will occur on cambered aerofoils

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7
Q

What are the 3 possible components to airflow over an aerofoil?

A

Chordwise
Spanwise
Vertical

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8
Q

Describe an infinite aerofoil

A

Only has flow in 2 dimensions… chordwise and vertical.
Has no wingtip (elliptical) or is infinitely long. This is as these limit development of spanwise flow.
A high AR wing is considered infinite.
Are considered “idealised” wings.

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9
Q

Describe a finite aerofoil

A

Has airflow in all 3 dimensions.
Is a wing with a limited wingspan or with a wingtip.
Are considered “real” wings.

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10
Q

Explain how Bernoulli’s theorem explains the production of lift.
Include any limitations

A

Ps+Pd=Pt
Airflow in streamline speeds up over the wing and reduces below.
As a result pressure reduces above the wing increases below the wing and a/c is sucked up into this region of low pressure.
Limitations include:
-only considers 1 dimension (chordwise)
—>no vertical as any elevation is insignificant compared to the size of the a/c… so assumes level flow and no spanwise flow
-all limitations of benoullis theorem discussed earlier
-no boundary layer seperation
-unable to explain up/downwash

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11
Q

Explain how Newton’s theorem (momentum/impulse) explains the production of lift.
Include any limitations

A

It states the net force on an object is equal to the rate of change of momentum and utilises Newton’s 3rd law (equal/opposite).
Horizontal air velocity is equal before/after aerofoil so there is no overall momentum change so therefore no horizontal force component on the airstream.
There is a change of momentum in the vertical plane, as the vertical component, w, changes direction by 180* because of up/down wash (but assumed magnitude remains equal). So Ft=mv can be rewritten as Ft=-2mw (think of ball against wall example). So impulse is x2 momentum in vertical direction… the - means the direction of the force is downwards. If Newton’s 3rd is applied, the reaction force of the airflow gives to the aerofoil (upward) = the force the aerofoil produced by deflecting the airflow downward.
Refer to notes for variables of equations explained.
Limitations include:
-2D flow (does not explain spanwise flow)
-Flow must be non viscous
-Flow must not seperate

-However compared to Bernoulli’s theorem it recognises up/downwash as contributing to lift production.

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12
Q

Do we need to know about Euler’s & Navier Stokes equation?

A

Nooooooooope.

Just that it explains 3D flow and requires supercomputers to solve partial differential equations.

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13
Q

Explain the how there is a circulation in the circulation theory of lift

A

It can be assumed the freestream air velocity is horizontal and uniform and that an object travels at a constant speed.
So… (refer to notes for the labels for each bullet point)
-upwash is the Vfs+small vertical velocity
-local air velocity above the aerofoil is Vfs+small horizontal velocity
-downwash is the Vfs-small vertical velocity
-local air velocity below the aerofoil is Vfs-small horizontal velocity
So if we superimpose the 2 air flows (uniform horizontal airflow where V=Vfs and the circulation) we get the streamlined flow of air over an aerofoil (refer notes for diagram)

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14
Q

List the assumptions with the circulation theory of lift

A
  • object travels at a constant speed
  • MUST be of a thin & symmetrical infinite aerofoil
  • air particles leave the TE evenly (uniform) downward
  • does not account for boundary layer separation
  • does not account for friction
  • must apply a superposition
  • 2D flow of air only (no spanwise)
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15
Q

What is the equation for circulation?

Do the air particles rotate?

A

C= V x path C=m^2s^-1. But in exam use the funny symbol one which you will need to refer to notes for. Note C has a unique symbol.

No, although there is a circulation in the airstream the air particles are irrotational (do not rotate).

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16
Q

Explain how the Kuta Joukowski theorem links to the circulation theory of lift

A

The theorem states “force per unit length acting at right angles to the airstream is equal to the product of the air density, air velocity and circulation (F=CpV in Nm-1)”
Lift per wingspan L=pVC
Induced drag per wingspan D=pwC

17
Q

What does each finger represent in the RH rule when applying KJ theorem?

A

Thumb: direction of force
Index: direction of airspeed/velocity
Middle: direction of circulation… find this but curling fingers in direction of circulation on RH & thumb is the direction of circulation

18
Q

Which way does the force act on the airflow “over” the aerofoil?
What about on a basketball that has been shot?

A

Upward

Upward

19
Q

What is the diameter of circulation assumed to be?
What equation do we get as a result?
How can this be used to derive L=pvw x Pi x S ?

A

Diameter approximates chord… then downwash is proportional to circulation
So C=w x Pi x C (w velocity and circulation/circumference is piC)

kJ states F=L=CpV
If C=wc x Pi 
L=pV x wcPi ... across wingspan b
L=Cl x 0.5pv^2 x S= pVw x Pi x S
Where c is chord & C is circulation
20
Q

What is Cl and CD equal too? What are they approximate to? (inc AoA).
How are the two proportional?

A

Cl= (2 x Pi x w)/V = 2 x Pi x AoA. So Cl prop AoA
CD= (2 x Pi x w^2)/V^2 = 2 x Pi x AoA^2
Where AoA is in RADIANS and is approximates w/v when AoA is small on a thin symmetrical aerofoil. This is explained in pencil in notes how this is achieved.

CD prop Cl^2/Pi

21
Q

What equations of KJ theorem allow for wing geometry (camber/AR etc)?

A

Cl= K x Pi (AoA0 + AoA) or Cl0 + 2K Pi AoA
Where AoA(0) is a zero lift AoA
Cl0 is Cl at 0 AoA
K(l) is related to aerofoil features (Thickness)

22
Q

What is the Cd due to downwash?

A
K x (Cl^2)/piAR      OR
Cl^2/piARe
Where k/e is a constant due to wing efficiency
23
Q

Does a symmetrical aerofoil have Cl?

A

Yes, but not at 0* AoA