SYE 3801 Aerodynamics Spring 2015 - KSU | Faculty...

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SYE 3801 Aerodynamics Spring 2015 Dr. Thomas Fallon Email: [email protected]

Transcript of SYE 3801 Aerodynamics Spring 2015 - KSU | Faculty...

Page 1: SYE 3801 Aerodynamics Spring 2015 - KSU | Faculty Webfacultyweb.kennesaw.edu/tfallon/sye3801/SYE3801_Lecture2... · 2015. 6. 6. · SYE 3801 - Aerodynamics - Spring 2015 12/16/2015

SYE 3801

Aerodynamics

Spring 2015

Dr. Thomas Fallon

Email: [email protected]

Page 2: SYE 3801 Aerodynamics Spring 2015 - KSU | Faculty Webfacultyweb.kennesaw.edu/tfallon/sye3801/SYE3801_Lecture2... · 2015. 6. 6. · SYE 3801 - Aerodynamics - Spring 2015 12/16/2015

Aerodynamics

• The science that deal with the flow of any gas

• Heavier than air machine can fly due to flow of air

over its surface

• Applications of aerodynamics;

• Rockets, jet engines, propeller, space vehicle, wind tunnels,

projectiles, motion of global atmosphere, flow of gases

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Review: Derivative and Differential ElementsRef: Calculus and Analytic Geometry, Thomas/Finney, Addison-Wesley Publishing Co., ISBN: 0-201-07540-7

𝑓′ 𝑥 =𝑑𝑦

𝑑𝑥= lim

Δ𝑥→0

𝑓 𝑥 + Δ𝑥 − 𝑓(𝑥)

Δ𝑥= 𝑚

Algorithm using f(x) = mx + b:

1. f(x + Δx) = m(x + Δx) + bf(x) = mx + b

2. Subtract: f(x + Δx) – f(x) = mΔx

3. Divide by Δx: f(x + Δx)−f(x)

Δx=

mΔ𝑥

Δ𝑥= 𝑚

4. Calculate limΔ𝑥→0

: f ′ x = limΔ𝑥→0

f(x + Δx)−f(x)Δx = 𝑚

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Example: For 𝑓 𝑥 = 𝑥2 +1

𝑥, derive 𝑓′ 𝑥 using the derivative algorithm

1. 𝑓 𝑥 + Δ𝑥 = 𝑥 + Δ𝑥 2 +1

(𝑥+Δ𝑥)= 𝑥2 + 2𝑥Δ𝑥 + (Δ𝑥)2+

1

(𝑥+Δ𝑥)

2. 𝑓 𝑥 = 𝑥2 +1

𝑥

3. Subtract: 𝑓 𝑥 + Δ𝑥 − 𝑓 𝑥 = 2𝑥Δ𝑥 + (Δ𝑥)2+1

(𝑥+Δ𝑥)−

1

𝑥

= 2𝑥Δ𝑥 + (Δ𝑥)2+𝑥−(𝑥+Δ𝑥)

𝑥(𝑥+Δ𝑥)= Δ𝑥 2x + Δ𝑥 −

1

𝑥 𝑥+Δ𝑥

4. Divide by Δ𝑥 : 𝑓 𝑥+Δ𝑥 −𝑓(𝑥)

Δ𝑥= 2x + Δ𝑥 −

1

𝑥 𝑥+Δ𝑥

5. Calculate limΔ𝑥→0

: 𝑓′ 𝑥 = limΔ𝑥→0

f(x + Δx)−f(x)Δx = lim

Δ𝑥→02x + Δ𝑥 −

1

𝑥 𝑥+Δ𝑥=

2𝑥 + 0 −1

𝑥 𝑥+0= 2𝑥 −

1

𝑥2

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Differential Elements

𝑑𝑦 = 𝑓′ 𝑥0 𝑑𝑥,𝑤ℎ𝑒𝑟𝑒 𝑑𝑥 𝑖𝑠 𝑎𝑛 𝑖𝑛𝑑𝑒𝑝𝑒𝑛𝑑𝑒𝑛𝑡 𝑣𝑎𝑟𝑖𝑎𝑏𝑙𝑒 𝑜𝑓 𝑐ℎ𝑎𝑛𝑔𝑒in the x−direction

𝑓𝑟𝑜𝑚 𝑥0,and dy is a dependent variable of change in the y-direction

to the tangential o𝑓𝑥0.

Example: For x = cos( 𝑡), 𝑦 = sin(𝑡), 𝑓𝑖𝑛𝑑𝑑𝑦

𝑑𝑥

𝑑𝑥 = −sin(𝑡)𝑑𝑡𝑑𝑦 = cos 𝑡 𝑑𝑡

𝑑𝑦

𝑑𝑥=

cos 𝑡 𝑑𝑡

−sin(𝑡)𝑑𝑡=

𝑥

−𝑦

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Pressure, ( )• Pressure = Force per unit area

“Pressure is the normal force per unit area exerted on a

surface due to the time rate of change of momentum

of the gas molecules impacting on that surface”

p = mv

dp/dt = m(dv/dt) = ma = F

P = F/A

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P

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Where;

dA = an incremental area around B

dF = Force on one side of dA due to pressure

0limdA

dFP

dA

Units:

2 2 2( ), ( ), ,

N lb dynepascal psi atm

m in cm

We apply pressure at point: points in a flow, hand outside car window

What about a thumbtack?

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Density, ( )

• Density = Mass per unit volume

“The density of a substance is the mass of that

substance per unit volume”

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Where;

dm = Mass of gas inside dV

dV = Elemental volume around point B

0limdV

dm

dV

Units:

*

3 3 3 3, , , mlbkg slug g

m ft cm ft

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Temperature, ( )

“The measure of average kinetic energy of the particles

of gas”

KE = 3/2kT, where k = Boltzmann constant (1.38 x 10-23 J/K)

K = 273.13 + C

Question: What does -120ºC equals to in degree Kelvin?

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Units:

( ), ( ), ( ), ( )Kelvin K Celsius C Rankine R Fahrenheit Fo o o

T

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Relationship between P, ρ, and T (all scalars)

is referred to the Equation of State

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Perfect Gas

“A perfect gas is one in which intermolecular forces are

negligible”

“Air under normal conditions (e.g. subsonic flight

through the atmosphere) behaves like a perfect gas”

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Perfect Gas

• Equation of state for a perfect gas

Where:

R = Specific gas constant

= 287 for air

= 1716 for air

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P RT

J kg K

( ) ( )ft lb slug R o

Specific Volume: ( ) is the

inverse density

1P RT RT

v

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P RTN/m2 = kg/m3 x J/(kg)(K) x K = J/m3

Are they equal?

True Equation of State is referred to as the Berthelot Equation:

P/ρRT = 1 + aP/T – bP/T3

As P decreases or as T increases the Berthelot Equation approaches the Equation of State

for a perfect gas.

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Compute the temperature of a point on a wing of an

Airbus A320, where the pressure and density are given

as 1.20 x 105 N/m2 and 1.1 kg/m3, respectively.

𝑃 = 𝜌𝑅𝑇 → 𝑇 =𝑃

𝜌𝑅=

1.20𝑥105 𝑁/𝑚2

1.1𝑘𝑔/𝑚3𝑥287𝐽/(𝑘𝑔)(𝑘)= 318°K = 45°C

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P, ρ, and T under standard conditions (sea level):

Ps = 1.01325 x 105 N/m2 = 1atm

ρs = 1.225 kg/m3

Ts = 288.15K

Compute the total air mass in a classroom with dimensions

30m x 20m x 3m at sea level under standard atmospheric

conditions.

ρ =𝑚

𝑉→ 𝑚 = 𝜌𝑉 =

1.225𝑘𝑔

𝑚3𝑥 30𝑚 𝑥 20𝑚 𝑥 3𝑚 = 2205𝑘𝑔

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Compute the density and specific volume of air in a wind

tunnel at P = 0.25atm and -120ºC

𝑃𝑣 = 𝑅𝑇 → 𝑣 =𝑅𝑇

𝑃=

287𝑥153

0.25𝑥1.01𝑥105=

1.74𝑚3

𝑘𝑔

𝜌 =1

𝑣=

0.57𝑘𝑔

𝑚3

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Given: Cabin pressure = 0.9 atm, T = 15°C, V = 1800m3 (of air). Air is recirculated every 20 minutes. Calculate the mass flow rate:

1atm = 1.01325 x 105N/M2

P = 0.9atm = 0.9x1.01325x105 = 0.909x105N/M2

T = 273 + 15 = 288Kρ = P/RT = 0.909x105/(287)(288) = 1.1kg/m3

Total mass m = ρV = (1.1)(1800) = 1980kgMass flow rate = m = 1980/1200 = 1.65kg/s

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Speed“Displacement per unit time”

“Speed + Direction”

- Vector quantity

- The velocity of gas may vary from point to point in a flow

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Units:

, ,km

mph machhrVelocity, ( )V

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Given: Baseball thrown by a pitcher at 85 mph. Calculate the minimum

and maximum velocity at the surface and their locations:

Theoretical expression of the field velocity:

V = 3/2V∞sinϴ, where V∞ = Free stream velocity

Flow (V∞ = 85 mph)

Vmin = 0 at ϴ = 0°; ie.e when ϴ = 0° and ϴ = 180°Vmax = 3/2(85)(1) = 127.5 mph at ϴ = 90°

ϴ

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Streamline

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“As long as the flow is steady (does not fluctuate with time) a moving fluid

element is seen to trace out a fixed path in space”

The path taken by a moving fluid element is called a streamline of a flow.

The velocity at point B is represented by an infinitesimally small element

of fluid as is moves through B; V is tangential to the streamline at point B.

V = ds/dt (m/s)Note the stagnation point where V = 0

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Streamline

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Laminar flow = low Reynolds number

Turbulent flow = high Reynolds number Small vortices of turbulence

Wind Tunnel Video: http://tinyurl.com/lq85lba

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Streamline

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Source of Aerodynamic Forces

“The knowledge of and at each point of a

flow fully defines the flow field”

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, ,P T V

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Source of Aerodynamic Forces

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Source of Aerodynamic Forces

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Pressure: always acts normal to

the surface

Shear stress: ( ) is the force

per unit area acting tangentially

on the surface due to friction.

The velocity decreases down

through the boundary layer as it

goes to 0 at the surface.

w

Which of the two forces contributes most to lift?

τw contributes more to lift at high α

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Standard International (SI) Units

• NACA (National Advisory Committee for Aeronautics) NASA

requires the use of SI units

• AIAA (American Institute of Aeronautics and Astronautics)

encourages the use of SI units

Length Mass Time Temp Pressure Density

SI m kg sec Kelvins N/m2 kg/m3

English foot slug sec Rankine lb/ft2 Slugs/ft3