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MAE 1202: AEROSPACE PRACTICUM
Lecture 5: Compressible and Isentropic Flow 1
February 11, 2013
Mechanical and Aerospace Engineering Department
Florida Institute of Technology
D. R. Kirk
READING AND HOMEWORK ASSIGNMENTS
• Reading: Introduction to Flight, by John D. Anderson, Jr.
– For this week’s lecture: Chapter 4, Sections 4.10 - 4.21, 4.27
– For next week’s lecture: Chapter 5, Sections 5.1 - 5.13
• Lecture-Based Homework Assignment:
– Problems: 4.7, 4.11, 4.18, 4.19, 4.20, 4.23, 4.27
• DUE: Friday, February 22, 2013 by 5 PM
– Problems: 5.2, 5.3, 5.4, 5.6
• DUE: Friday, March 1, 2013 by 5 PM
• Turn in hard copy of homework
– Also be sure to review and be familiar with textbook examples in Chapter 5
ANSWERS TO LECTURE HOMEWORK• 5.2: L = 23.9 lb, D = 0.25 lb, Mc/4 = -2.68 lb ft
– Note 1: Two sets of lift and moment coefficient data are given for the NACA 1412 airfoil, with and without flap deflection. Make sure to read axis and legend properly, and use only flap retracted data.
– Note 2: The scale for cm,c/4 is different than that for cl, so be careful when reading the data
• 5.3: L = 308 N, D = 2.77 N, Mc/4 = - 0.925 N m
• 5.4: = 2°
• 5.6: (L/D)max ~ 112
CREO DESIGN CONTEST
• Create most elaborate, complex, stunning Aerospace Related project in Creo
• Criteria: Assembly and/or exploded view
• First place
– Either increase your grade by an entire letter (C → B), or
– Buy your most expensive textbook next semester
• Second place: +10 points on final exam
• Third place: +10 points on final exam
CAD DESIGN CONTEST
CAD DESIGN CONTEST
If you do the PRO|E challenge…
Do not let it consume you!
BERNOULLI’S EQUATION
2
222
21
1
22
2
Vp
Vp
Vp
• One of most fundamental and useful equations in aerospace engineering!
• Remember:
– Bernoulli’s equation holds only for inviscid (frictionless) and incompressible (= constant) flows
– Bernoulli’s equation relates properties between different points along a streamline
– For a compressible flow Euler’s equation must be used ( is variable)
– Both Euler’s and Bernoulli’s equations are expressions of F = ma expressed in a useful form for fluid flows and aerodynamics
Constant along a streamline
13
EXAMPLE: MEASUREMENT OF AIRSPEED (4.11)• How do we measure an airplanes speed in flight?
• Pitot tubes are used on aircraft as speedometers (point measurement)
14
STATIC VS. TOTAL PRESSURE• In aerodynamics, 2 types of pressure: Static and Total (Stagnation)
• Static Pressure, p– Due to random motion of gas molecules– Pressure we would feel if moving along with flow– Strong function of altitude
• Total (or Stagnation) Pressure, p0 or pt
– Property associated with flow motion– Total pressure at a given point in flow is the pressure that would exist if flow were
slowed down isentropically to zero velocity
• p0 ≥ p
MEASUREMENT OF AIRSPEED: INCOMPRESSIBLE FLOW
02
12
1pVp
pp
V
01
2
Staticpressure
Dynamicpressure
Totalpressure
Incompressible Flow
Total and Static Ports
16
17
TOTAL PRESSURE MEASUREMENT (4.11)
• Measures total pressure
• Open at A, closed at B
• Gas stagnated (not moving) anywhere in tube
• Gas particle moving along streamline C will be isentropically brought to rest at point A, giving total pressure
18
EXAMPLE: MEASUREMENT OF AIRSPEED (4.11)• Point A: Static Pressure, p
– Only random motion of gas is measured
• Point B: Total Pressure, p0
– Flow is isentropically decelerated to zero velocity
• A combination of p0 and p allows us to measure V1 at a given point
• Instrument is called a Pitot-static probe p0
p
19
MEASUREMENT OF AIRSPEED: INCOMPRESSIBLE FLOW
02
12
1pVp
02
12
1pVp
pp
V
01
2
Staticpressure
Dynamicpressure
Totalpressure
Incompressible Flow
20
TRUE VS. EQUIVALENT AIRSPEED• What is value of ?
• If is measured in actual air around the airplane
• Measurement is difficult to do
• Practically easier to use value at standard seal-level conditions, s
• This gives an expression called equivalent airspeed
pp
Vtrue
02
s
e
ppV
02
TRAGIC EXAMPLE: Air France Crash
• Aircraft crashed following an aerodynamic stall caused by inconsistent airspeed sensor readings, disengagement of autopilot, and pilot making nose-up inputs despite stall warnings
• Reason for faulty readings is unknown, but it is assumed by accident investigators to have been caused by formation of ice inside pitot tubes, depriving airspeed sensors of forward-facing air pressure.
• Pitot tube blockage has contributed to airliner crashes in the past 21
HOW DOES AN AIRFOIL GENERATE LIFT?• Lift due to imbalance of pressure distribution over top and bottom surfaces of
airfoil (or wing)
– If pressure on top is lower than pressure on bottom surface, lift is generated
– Why is pressure lower on top surface?
• We can understand answer from basic physics:
– Continuity (Mass Conservation)
– Newton’s 2nd law (Euler or Bernoulli Equation)
Lift Force = PA
HOW DOES AN AIRFOIL GENERATE LIFT?1. Flow velocity over top of airfoil is faster than over bottom surface
– Streamtube A senses upper portion of airfoil as an obstruction
– Streamtube A is squashed to smaller cross-sectional area
– Mass continuity AV=constant: IF A↓ THEN V↑
Streamtube A is squashedmost in nose region(ahead of maximum thickness)
AB
HOW DOES AN AIRFOIL GENERATE LIFT?2. As V ↑ p↓
– Incompressible: Bernoulli’s Equation
– Compressible: Euler’s Equation
– Called Bernoulli Effect
3. With lower pressure over upper surface and higher pressure over bottom surface, airfoil feels a net force in upward direction → Lift
VdVdp
Vp
constant2
1 2
Most of lift is producedin first 20-30% of wing(just downstream of leading edge)
Can you express these ideas in your own words?
Incorrect Lift Theory• http://www.grc.nasa.gov/WWW/k-12/airplane/wrong1.html
SUMMARY OF GOVERNING EQUATIONS (4.8)
222
211
2211
2
1
2
1VpVp
VAVA
• Steady, incompressible flow of an
inviscid (frictionless) fluid along a streamline or in a stream tube of varying area
• Most important variables: p and V
• T and are constants throughout flow
continuity
Bernoulli
What if flow is high speed, M > 0.3?
What if there are temperature effects?
How does density change?
1st LAW OF THERMODYNAMICS (4.5)
System
e (J/kg)
Boundary
Surroundings
• System (gas) composed of molecules moving in random motion
• Energy of molecular motion is internal energy per unit mass, e, of system
• Only two ways e can be increased (or decreased):
1. Heat, q, added to (or removed from) system
2. Work, w, is done on (or by) system
THOUGHT EXPERIMENT #1
• Do not allow size of balloon to change (hold volume constant)
• Turn on a heat lamp
• Heat (or q) is added to the system
• How does e (internal energy per unit mass) inside the balloon change?
THOUGHT EXPERIMENT #2
• *You* take balloon and squeeze it down to a small size
• When volume varies work is done
• Who did the work on the balloon?
• How does e (internal energy per unit mass) inside the balloon change?
• Where did this increased energy come from?
1st LAW OF THERMODYNAMICS (4.5)
• System (gas) composed of molecules moving in random motion• Energy of all molecular motion is called internal energy per unit mass, e, of
system
• Only two ways e can be increased (or decreased):1. Heat, q, added to (or removed from) system2. Work, w, is done on (or by) system
SYSTEM(unit mass of gas)
Boundary
SURROUNDINGS
q
wqde
e (J/kg)
1st LAW IN MORE USEFUL FORM (4.5)
• 1st Law: de = q + w– Find more useful expression for w, in
terms of p and (or v = 1/)
• When volume varies → work is done• Work done on balloon, volume ↓• Work done by balloon, volume ↑
pdvqde
wqde
pdvw
sdAppsdAw
spdA
AA
ΔW
distanceforceΔW
Change inVolume (-)
ENTHALPY: A USEFUL QUANTITY (4.5)
vdpdhq
vdpdedhdeq
pdvdeq
vdppdvdedh
RTepveh
Define a new quantitycalled enthalpy, h:(recall ideal gas law: pv = RT)
Differentiate
Substitute into 1st law(from previous slide)
Another version of 1st lawthat uses enthalpy, h:
HEAT ADDITION AND SPECIFIC HEAT (4.5)
• Addition of q will cause a small change in temperature dT of system
• Specific heat is heat added per unit change in temperature of system
• Different materials have different specific heats
– Balloon filled with He, N2, Ar, water, lead, uranium, etc…
• ALSO, for a fixed dq, resulting dT depends on type of process…
Kkg
J
dT
qc
q
d
SPECIFIC HEAT: CONSTANT PRESSURE• Addition of q will cause a small change in temperature dT of system• System pressure remains constant
Tch
dTcdh
dTcq
dT
qc
p
p
p
p
pressureconstant
q
d
Kkg
J
dT
qc
Extra Credit #1:Show this step
SPECIFIC HEAT: CONSTANT VOLUME• Addition of q will cause a small change in temperature dT of system• System volume remains constant
Kkg
J
dT
qc
q
d
Tce
dTcde
dTcq
dT
qc
v
v
v
v
olumeconstant v
Extra Credit #2:Show this step
HEAT ADDITION AND SPECIFIC HEAT (4.5)
• Addition of q will cause a small change in temperature dT of system
• Specific heat is heat added per unit change in temperature of system
Tch
dTcdh
dTcq
dT
qc
p
p
p
p
pressureconstant
• However, for a fixed dq, resulting dT depends on type of process:
Tce
dTcde
dTcq
dT
qc
v
v
v
v
olumeconstant v
Kkg
J
dT
qc
v
p
c
c
Specific heat ratioFor air, = 1.4
Constant Pressure Constant Volume
ISENTROPIC FLOW (4.6)• Goal: Relate Thermodynamics to Compressible Flow
• Adiabatic Process: No heat is added or removed from system
– q = 0
– Note: Temperature can still change because of changing density
• Reversible Process: No friction (or other dissipative effects)
• Isentropic Process: (1) Adiabatic + (2) Reversible
– (1) No heat exchange + (2) no frictional losses
– Relevant for compressible flows only
– Provides important relationships among thermodynamic variables at two different points along a streamline
1
1
2
1
2
1
2
T
T
p
p = ratio of specific heats= cp/cv
air=1.4
DERIVATION: ENERGY EQUATION (4.7)
022
0
0
0
0
0
21
22
12
2
1
2
1
VVhh
VdVdh
VdVdh
VdVvdh
VdVdp
vdpdhq
q
wqde
V
V
h
h
Energy can neither be created nor destroyedStart with 1st law
Adiabatic, q=01st law in terms of enthalpy
Recall Euler’s equation
Combine
Integrate
Result: frictionless + adiabatic flow
ENERGY EQUATION SUMMARY (4.7)• Energy can neither be created nor destroyed; can only change physical form
– Same idea as 1st law of thermodynamics
constant2
222
22
2
21
1
Vh
Vh
Vh
constant2
222
22
2
21
1
VTc
VTc
VTc
p
pp
Energy equation for frictionless,adiabatic flow (isentropic)
h = enthalpy = e+p/= e+RTh = cpT for an ideal gas
Also energy equation forfrictionless, adiabatic flow
Relates T and V at two different points along a streamline
SUMMARY OF GOVERNING EQUATIONS (4.8)STEADY AND INVISCID FLOW
222
211
2211
2
1
2
1VpVp
VAVA
222
111
222
211
1
2
1
2
1
2
1
222111
2
1
2
1
RTp
RTp
VTcVTc
T
T
p
p
VAVA
pp
• Incompressible flow of fluid along a streamline or in a stream tube of varying area
• Most important variables: p and V
• T and are constants throughout flow
• Compressible, isentropic (adiabatic and frictionless) flow along a streamline or in a stream tube of varying area
• T, p, , and V are all variables
continuity
Bernoulli
continuity
isentropic
energy
equation of stateat any point
EXAMPLE: SPEED OF SOUND (4.9)• Sound waves travel through air at a finite speed
• Sound speed (information speed) has an important role in aerodynamics
• Combine conservation of mass, Euler’s equation and isentropic relations:
RTp
a
a
VM
• Speed of sound, a, in a perfect gas depends only on temperature of gas
• Mach number = flow velocity normalizes by speed of sound
– If M < 1 flow is subsonic
– If M = 1 flow is sonic
– If M > flow is supersonic
• If M < 0.3 flow may be considered incompressible
ddp
a 2
KEY TERMS: CAN YOU DEFINE THEM?
• Streamline
• Stream tube
• Steady flow
• Unsteady flow
• Viscid flow
• Inviscid flow
• Compressible flow
• Incompressible flow
• Laminar flow
• Turbulent flow
• Constant pressure process
• Constant volume process
• Adiabatic
• Reversible
• Isentropic
• Enthalpy
MEASUREMENT OF AIRSPEED:SUBSONIC COMRESSIBLE FLOW
• If M > 0.3, flow is compressible (density changes are important)
• Need to introduce energy equation and isentropic relations
21
1
0
1
21
1
0
02
11
2
11
21
2
1
MT
T
Tc
V
T
T
TcVTc
p
pp
11
21
1
0
12
11
0
2
11
2
11
M
Mp
p
cp: specific heat at constant pressureM1=V1/a1
air=1.4
MEASUREMENT OF AIRSPEED:SUBSONIC COMRESSIBLE FLOW
• So, how do we use these results to measure airspeed
111
2
111
2
11
2
11
2
1
102
2
1
1
10212
1
1
1
0212
1
1
1
021
s
scal p
ppaV
p
ppaV
p
paV
p
pM
p0 and p1 giveFlight Mach numberMach meter
M1=V1/a1
Actual Flight Speed
Actual Flight Speedusing pressure difference
What is T1 and a1?Again use sea-level conditions Ts, as, ps (a1=340.3 m/s)
EXAMPLE: TOTAL TEMPERATURE
• A rocket is flying at Mach 6 through a portion of the atmosphere where the static temperature is 200 K
• What temperature does the nose of the rocket ‘feel’?
• T0 = 200(1+ 0.2(36)) = 1,640 K!
21
1
0
2
11 M
T
T
Total temperature
Static temperature Vehicle flightMach number
MEASUREMENT OF AIRSPEED:SUPERSONIC FLOW
• What can happen in supersonic flows?
• Supersonic flows (M > 1) are qualitatively and quantitatively different from subsonic flows (M < 1)
HOW AND WHY DOES A SHOCK WAVE FORM?
• Think of a as ‘information speed’ and M=V/a as ratio of flow speed to information speed
• If M < 1 information available throughout flow field
• If M > 1 information confined to some region of flow field
MEASUREMENT OF AIRSPEED:SUPERSONIC FLOW
1
21
124
1 21
1
21
21
2
1
02
M
M
M
p
p
Notice how different this expression is from previous expressionsYou will learn a lot more about shock wave in compressible flow course
SUMMARY OF AIR SPEED MEASUREMENT
• Subsonic, incompressible
• Subsonic, compressible
• Supersonic
1
21
124
1 21
1
21
21
2
1
02
M
M
M
p
p
111
21
102
2
s
scal p
ppaV
s
e
ppV
02
HOW ARE ROCKET NOZZLES SHAPPED?
MORE ON SUPERSONIC FLOWS (4.13)
V
dVM
A
dAV
dV
A
dA
a
VdV
V
dV
A
dA
dp
VdVd
VdVdp
V
dV
A
dAd
AV
1
0
0
0
constantlnlnVlnAln
constant
2
2
Isentropic flow in a streamtube
Differentiate
Euler’s Equation
Since flow is isentropica2=dp/d
Area-Velocity Relation
CONSEQUENCES OF AREA-VELOCITY RELATION
V
dVM
A
dA12
• IF Flow is Subsonic (M < 1)
– For V to increase (dV positive) area must decrease (dA negative)
– Note that this is consistent with Euler’s equation for dV and dp
• IF Flow is Supersonic (M > 1)
– For V to increase (dV positive) area must increase (dA positive)
• IF Flow is Sonic (M = 1)
– M = 1 occurs at a minimum area of cross-section
– Minimum area is called a throat (dA/A = 0)
TRENDS: CONTRACTION
M1 < 1
M1 > 1
V2 > V1
V2 < V1
1: INLET 2: OUTLET
TRENDS: EXPANSION
M1 < 1
M1 > 1
V2 < V1
V2 > V1
1: INLET 2: OUTLET
PUT IT TOGETHER: C-D NOZZLE
1: INLET 2: OUTLET
MORE ON SUPERSONIC FLOWS (4.13)
• A converging-diverging, with a minimum area throat, is necessary to produce a supersonic flow from rest
Supersonic wind tunnel section Rocket nozzle
SUMMARY OF GOVERNING EQUATIONS (4.8)STEADY AND INVISCID FLOW
222
211
2211
2
1
2
1VpVp
VAVA
222
111
222
211
1
2
1
2
1
2
1
222111
2
1
2
1
RTp
RTp
VTcVTc
T
T
p
p
VAVA
pp
• Incompressible flow of fluid along a streamline or in a stream tube of varying area
• Most important variables: p and V
• T and are constants throughout flow
• Compressible, isentropic (adiabatic and frictionless) flow along a streamline or in a stream tube of varying area
• T, p, , and V are all variables
continuity
Bernoulli
continuity
isentropic
energy
equation of stateat any point