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AEROCFD ROCKET:
INSTRUCTIONS BACK
The V-2 rocket
is used to illustrate the step-by-step procedure necessary to
perform a typical analysis using AeroCFD. Initially, the user
specifies the analysis units and flight conditions on the main
page of the program. The following steps are required on the main
screen to perform an analysis using AeroCFD. Please read the definitions section for explanation of
each variables meaning.
1) For the Analysis Units data entry specify whether the
required units are inches-pounds-seconds (IPS), feet-pounds-seconds
(FPS), or meters-newtons-seconds (MNS) by using
the pull-down menu control. Depending on the selection, the resulting
units are inches, feet or meters for linear dimensions, pounds
or Newtons for force and seconds for the basic units of time.
Select IPS for this example.
2) In the Analysis Data section specify the Rocket Flight
Speed as either IN/SEC, FT/SEC, M/SEC
or MACH number using the pull-down menu. Select MACH
for this example and for Rocket Flight Speed insert
0.25 Mach.
3) In the Analysis Data section specify the Rocket AOA
(angle of attack) in degrees by inserting the data entry. Insert
1.0 degree AOA for this example.
4) In the Analysis Data section specify the Rocket Flight
Altitude using the pull-down menu. Select SEA LEVEL for
this example.
5) In the Analysis Data section specify whether the fluid
is COMPRESSIBLE or INCOMPRESSIBLE using the pull-down
menu. The INCOMPRESSIBLE selection allows AeroCFD to perform
a 3-D potential flow analysis. The COMPRESSIBLE flow selection
allows AeroCFD to apply a linearized compressibility correction
(using the Prandtl-Glauret rule) to the 3-D potential flow results.
The Prandtl-Glauret rule is reasonably accurate for 0.3 < M
< 0.8. However, for M > 0.8 the accuracy of the Prandtl-Glauret
rule diminishes rapidly. Select COMPRESSIBLE for this example.
6) In the Analysis Data section specify the Mesh Size
of the computational flow field in the axial (X) and transverse
(Y) directions using the pull-down menu. The size of the computational
flow field can range from 10 X 10 elements to 100 X
100 elements. More elements yield more accuracy but add to
the total computational time for a solution. Insert 50 for
this example.
7) In the Analysis Data section specify the Element
Aspect Ratio as 1:1, 2:1, 3:1, or 4:1.
Increasing the element aspect ratio is useful to cluster the mesh
around the body tube and to get better plot resolution in regions
where the flow velocity and pressure are changing rapidly. Clustering
elements in regions where the flow is changing rapidly is especially
important for accurate line-contour plots and filled-contour plots.
Select 1 for this example. Note: "mesh" refers
to a grouping of grids.
8) In the Analysis Data section specify the Grid # on
Circumference as either 8, 10 or 12.
The default of 8 panel control points on the circumference
is fine for most analyses. But, more panels control points on
the circumference will yield better accuracy. Select 8 for
this example.
9) The user must dimension the body tube to be able to perform
a CFD solution. "Click" the first icon at the top of
the main screen to bring up the Body Tube Geometry screen.
Prior to specifying body tube geometry, clicking anywhere else
on the main screen will cause AeroCFD to display error messages
in the status bar at the bottom of the screen. These messages
indicate what AeroCFD needs to proceed to the next step of the
analysis.
Note: CX refers to the drag force coefficient in the axial direction
of the airframe and CY (CN) refers to the lift force coefficient
perpendicular to the axial direction of the airframe. CD refers
to the drag force coefficient in the flow direction and CL refers
to the lift force coefficient perpendicular to the flow direction.
Please click the first
(Body Tube Geometry), second (Fin Geometry), third
(Flow Visualization) and forth (Force Distribution) icons
in the toolbar. Please click SHOW RESULTS / SHOW ANALYSIS
button to view either the CFD Results or the Analysis Data sections.
The "X" command
button on the AeroCFD
toolbar hides or shows the Analysis Data and CFD Results
sections.
Main AeroCFD screen - Analysis
Input
Main AeroCFD screen - CFD
Results
BODY TUBE GEOMETRY
To generate a "Standard"
body tube perform the following sequence of operations.
10) On the main AeroCFD screen "click" the first icon
on the toolbar to bring up the Body Tube Geometry screen.
In the Body Tube Geometry section select the Standard
Tube Geometry option button. Selecting the Free-Form Tube
Geometry will display the Free-Form Body Tube Geometry
screen. However, these V-2 rocket instructions will use the "Standard"
method to create the body tube for this illustration. "Click"
the subdued Free-Form icon for instructions
to see what the Free-Form Body Tube Geometry screen looks
like . To use the Free-Form Body Tube Geometry screen,
simply select the number of points describing the body tube using
the up-down control. Then "drag" each point into position
on the screen. Better point resolution is possible by resizing
the window to fit the entire computer screen by clicking the RESIZE
command.
11) In the FREE-FORM AND STANDARD GEOMETRY DATA section
specify the nose cone shape as CONICAL, ELLIPTICAL,
PARABOLIC, SEARS-HAACK, or TANGENT OGIVE.
The SEARS-HAACK nose cone has an up-down control that applies
a power-series shape modification. When the Shape index is equal
to 2 a SEARS-HAACK nose cone is defined and for other values
of Shape index a power series shape is defined. Select TANGENT
OGIVE for this example.
12) For Nose Cone Length insert 208.5 inches.
13) For Nose Cone Diameter insert 65.0 inches.
14) For Body Tube Length insert 185.0 inches.
15) In the FREE-FORM AND STANDARD GEOMETRY DATA section
specify the Transition shape as either CONICAL, ELLIPTICAL,
PARABOLIC, or TANGENT OGIVE. The aft end of the
V-2 is defined by a Tangent Ogive shape. Select Tangent Ogive
for the Transition Shape.
16) For Transition Diameter insert 40.9 inches.
17) For Transition Length insert 142.9 inches.
The Base Tube Length may be ignored for this example.
18) "Click" back to the main AeroCFD screen by "clicking"
the fifth icon on the toolbar.
Please remember that you need to "click" back using
the Return icon. Clicking the [X] box will kill the results
and delete the modifications.
Note: To generate a Free-Form body
tube shape click "Free-Form Tube Geometry" to
enable the Free-Form command button. Click on the Free-Form command
button to proceed to the Free-Form Geometry screen.
Please click the fifth (Return) icon in the toolbar
to return to the main screen.
Body Tube Geometry Screen
FIN AND LAUNCH
LUG GEOMETRY
To define the fins of
the V-2 rocket perform the following sequence of operations.
19) On the main AeroCFD screen "click" the second icon
on the toolbar to bring up the Fin and Launch Lug Geometry
screen.
20) In the Fin Quantity and Type section select the total
number of fins as 3, 4, 5, 6, 7,
or 8. Alternatively, any number of fins may be specified
by simply inserting the desired number of fins. Insert 3
fins for this example.
21) In the Fin Quantity and Type section select the option
button corresponding to either Main Fins or the Canard
Fins. The Main Fins are the lowest most set of fins
on the rocket and the Canard Fins are the upper most set
of fins on the rocket. For this example select the Main Fins
option button.
22) In the Fin Planform Shapes section select the option
button corresponding to either Triangle, Rectangle,
Tapered, or Elliptical fin planforms. For this example
select the Tapered planform fin shape.
23) In Airfoils Sections select the option button corresponding
to either Square, Round, Streamlined, or
D'Wedge cross-sectional fin shape. The fin cross-sectional
shape determines the drag and lift characteristics that are computed
in the 2-D vortex panel analysis for the fins. An average span
of the fin is used in the 2-D vortex panel fin analysis. For complex
fin designs the user must enter values that approximate the root
chord, fin tip chord, span length and fin thickness of the actual
fins. For this example select the Streamlined airfoil section.
24) In the Surface Finish section select the option button
corresponding to either None (unpainted), Good (painted),
or Excellent (waxed) for the surface finish of the entire
model rocket. This selection determines whether the flow on the
rocket body and fins are either laminar or turbulent when determining
the drag coefficients. Whether the flow is laminar or turbulent
flow is determined by the Reynolds number (Rn) which of course
is based on the flow velocity (V), dynamic viscosity and characteristic
length (L). For a body tube the characteristic length is the total
rocket length, and for fins the characteristic length is always
the average fin chord. As for all aerodynamic coefficients (Cd,
CL, etc.) the reference area (S) is either the cross-sectional
area immediately behind the nose cone or the maximum cross-sectional
area of the body tube. The selection for finish quality applies
to fins and body tube and launch lug. For this example select
Good (painted) for the surface finish.
25) Finally, insert all the remaining fin dimensions and launch
lug dimensions into each data entry area on the screen. The relative
location of each dimension is indicated when each fin planform
type is selected using the option buttons. For defining multiple
launch lugs the total length of all the launch lugs on the body
tube should be inserted for Total Length in the Launch
Lug(s) section. In addition, for non-circular launch lugs
compute the equivalent inside and outside circular diameter of
the launch lug. Then, insert the launch lug's equivalent outside
diameter into the Outside Diameter data field and the equivalent
inside diameter into the Inside Diameter data field.
The total length of the body tube determines if the flow over
the lug is laminar or turbulent when computing drag coefficients.
For this example insert 393.5" for the distance from
the nose cone tip to the leading edge of the fin root. Insert
449.96" for the distance from the nose cone tip to
the leading edge of the fin tip. Insert 102.6" for
the tip chord of the fin, insert 37.65" for the semi-span
of the fin. insert 142.9" for the root chord of the
fin. Insert 3.75" for average fin thickness. Insert
0.0" for the Total Length of the launch lug.
Insert 0.0" for the Outside Diameter of the
launch lug. Insert 0.0" for the Inside Diameter
of the launch lug. Note: most model rockets have launch lugs,
but the V-2 rocket does not.
26) "Click" back to the main AeroCFD screen by "clicking"
the fifth icon on the toolbar.
Please remember that you need to "click" back using
the Return icon. Clicking the [X] box will kill the results
and delete the modifications.
27) When the body tube geometry and fin geometry are complete
the user may "click" SOLVE to perform a CFD analysis,
"click" MESH to see the resulting flow field
grid, "click" LOOP to perform a CFD Loop Analysis
with or without the fins or "click" STOP to stop
the solution or proceed with a solution.
Please click the second (XML File Fin Geometry and Fin
Placement), forth icon (Fin AeroDynamics) and fifth (Return)
icons in the toolbar.
Fin Geometry Screen
FREE-FIELD FLOW VISUALIZATION
Flow visualization is
easy using AeroCFD. To plot the free-field flow in AeroCFD perform
the following sequence of operations after the flow is
SOLVE'd.
28) On the main AeroCFD screen "click" the third icon
on the toolbar to bring up the Flow Visualization screen.
29) To plot velocity filled-contour plots or velocity line-contour
plots in the Plot Velocity section "click" either
the Field-Filled or Field-Lines command buttons.
Plots will occur automatically.
30) Adjust the number of levels displayed in the contour plots
by using the up-down control to set the number of color levels
from a minimum of 3 to a maximum of 256.
31) To plot pressure filled-contour plots or pressure line-contour
plots in the Plot Pressure section "click"
either the Filled-Field or Field-Lines command buttons.
All plots will occur automatically and be displayed
in real-time. Plot dynamic pressure, static pressure or pressure
coefficient (Cp) by selecting one of the option buttons listed
in the Plot Pressure section. Please see the definitions
section for more information about dynamic pressure, static pressure
and pressure coefficient (Cp).
32) Adjust the number of levels displayed in the contour plots
by using the up-down control to set the number of color levels
from a minimum of 3 to a maximum of 256.
33) "Click" back to the main AeroCFD screen by "clicking"
the third icon on the toolbar.
Please remember that you need to "click" back using
the Return icon. Clicking the [X] box will kill the results
and delete the modifications.
Please click the third (Return) icon in the toolbar
or click SHOW PROFILES to view the velocity profile toolbar.
The "X" command
button on the AeroCFD
toolbar hides or shows the Contour Plot and Profiles
sections.
Flow Visualization Screen
Flow Visualization Screen
- [X] Button Clicked Showing Levels Display
AIRFRAME SURFACE FLOW FIELD VISUALIZATION
Flow visualization on
the surface of the airframe is easy using AeroCFD. To plot the
airframe flow field in AeroCFD perform the following sequence
of operations after the flow is SOLVE'd and the
Flow Visualization screen is displayed.
34) To plot airframe velocity filled-contour plots in the
Plot Velocity section "click" the Airframe-Filled
command button. The Plot will occur automatically.
35) Adjust the number of levels displayed in the contour plot
by using the up-down control to set the number of color levels
from a minimum of 3 to a maximum of 256.
36) To plot airframe pressure filled-contour plots in the
Plot Pressure section "click" the Airframe-Filled
command button. The plot will occur automatically.
Plot dynamic pressure, static pressure or pressure coefficient
(Cp) by selecting one of the option buttons listed in the Plot
Pressure section. Please see the definitions
section for more information about dynamic pressure, static pressure
and pressure coefficient (Cp).
37) Adjust the number of levels displayed in the contour plots
by using the up-down control to set the number of color levels
from a minimum of 3 to a maximum of 256.
38) View the profile plots by clicking the SHOW PROFILES
command button.
39) Plots may be interrupted or stopped by "clicking"
the STOP command button.
AIRFRAME POINT-PROPERTY DISPLAY
40)
Display control point
velocity or pressure and X,Y,Z panel control point coordinates
for each three-dimensional source panel on the surface of the
airframe. After the Airframe-Filled command button has
plotted either velocity or pressure on the surface of the airframe,
the Airframe Values section appears. The Airframe Values
section makes available the up/down command button that allows
the user to display control point values for velocity, dynamic
pressure, static pressure and pressure coefficient (Cp). Control
point coordinates are displayed in the status bar at the lower-left
part of the screen. As the up/down command button is clicked a
red dot on the surface of
the airframe moves from point-to-point in real-time displaying
either velocity or pressure depending on whether the airframe
plot was generated in the Plot Velocity or the Plot
Pressure sections. But, the user must first plot the airframe
filled-contours, either velocity or pressure to expose this utility
and make the Airframe Values section visible. This X,Y,Z
coordinates on the airframe use a right handed coordinate system.
The X-axis is down the axis of the rocket from the tip of the
nose cone, the Y-axis is up and the Z-axis points out from the
surface of the screen. A small coordinate system located on the
lower left of the screen makes the coordinate system clear. For
added clarity a sketch in the figure below shows a cross-sectional
view of the airframe and the resulting Y-Z axis that appears when
looking at the rocket from the front. Panel control point 109
represents one of 12 control points on the surface of the airframe
at this particular cross-sectional location. In this representation
the number of panel control points on the circumference of the
airframe was increased to 12 points. The V-2 example used 8 panel
control points on the circumference but 10 panel control points
on the circumference could have been selected in step 8.
Please
click the third (Return) icon in the toolbar or
click SHOW PROFILES to view the velocity profile toolbar.
The "X" command
button on the AeroCFD
toolbar hides or shows the Contour Plot and Profiles
sections.
Airframe Surface Flow Field
- Dynamic
Pressure Filled-Contour Plot
Airframe Point Property Display
VELOCITY AND PRESSURE
PROFILES PLOT
41) View the profile plots
by clicking the SHOW PROFILES command button.
42) Plots may be interrupted or stopped by "clicking"
the STOP command button.
43) Velocity and pressure variation from the surface of the model
in the vertical direction is displayed on the Profiles - Velocity
and Pressure section. The slider bar determines the
location of the pressure profile plot along the axis of the model.
The zero axial location is defined at the tip of the nose cone.
44) "Click" back to the main AeroCFD screen by "clicking"
the third icon on the toolbar.
Please remember that you need to "click" back using
the Return icon. Clicking the [X] box will kill the results
and delete the modifications.
NOTE: The vertical velocity or pressure profile at each X-Location
from the flow inlet to the end of the rocket is being plotted
each time the slider bar is moved. By definition, the tip of the
nose cone is the origin (X = 0, Y = 0) and the flow inlet (left
most part of the flow field) has a negative X-Location. Depending
on the number of grids selected in the X and Y directions, AeroCFD
needs to proportion the grid spacing along the airframe to put
the proper number of grids on the airframe for each mesh size
selected. The physical locations of the vertical profiles are
located at panel control points and not the intersections of the
grid lines. For this reason, properties are not displayed at the
tip of the nose cone where X =0 and Y =0, but a half panel width
away for the first profile section.
Please click the third (Return) icon in the toolbar
or SHOW CONTOURS to view the contour plot toolbar. The
"X" command
button on the AeroCFD
toolbar hides or shows the Contour Plot and Profiles
sections.
Profiles Screen
ROCKET FORCE DISTRIBUTION
A complete list of all
the aerodynamic coefficients, forces and moments can be viewed
by clicking the forth icon on the AeroCFD main screen toolbar.
The data on the Rocket Force Distribution screen includes
the aerodynamic data presented on the main page of the analysis
and much more.
45) After reviewing the Rocket Force Distribution screen
"Click" back to the main AeroCFD screen by "clicking"
the forth icon on the toolbar.
Please remember that you need to "click" back using
the Return icon. Clicking the [X] box will kill the results
and delete the modifications.
Please click the third (Cross-Flow Cp Distribution)
and forth (Return) icons in the toolbar.
Results Summary Screen
XML FILE FIN GEOMETRY AND FIN
PLACEMENT
This screen presents the
XML File Fin Geometry and Fin Placement screen. XML
fin data for a two stage rocket is displayed below after being
imported from the XML data file. Perform the following
sequence of operations to import fin data from an XML
file. These steps are not part of the V-2 rocket instructions.
However, if Free-Form fins are desired the user may import them
from an XML file. AeroCFD then determines the average fin
chord, etc. and inserts that information into the analysis.
1) On the Fin Geometry screen "click" the second
icon on the toolbar to bring up the XML File Fin Geometry and
Fin Placement screen.
2) In the XML File Fin Geometry and Fin Placement screen,
"Click" the left icon in the toolbar to import XML
custom or XML standard fins.
3) Using the option buttons, select the fin-set that needs to
be re-positioned.
4) Pull the slider-bar to position each fin set.
5) Units may be modified using the Fin Units pull-down
menu. These units are reflected on this screen and on the Fin
Geometry screen.
6) "Click" back to Fin Geometry screen by "clicking"
the fifth icon on the toolbar. Then "click" back to
the main AeroCFD screen.
Please remember that you need to "click" back using
the Return icon. Clicking the [X] box will kill the results
and delete the modifications.
Note: This screen does not represent the V-2 rocket example. It
is being provided for illustration and description.
Please click the fifth (Return) icon in the toolbar.
XML File Fin Geometry And Placement
Screen
CFD LOOP ANALYSIS
AND PLOTS
To perform a CFD Looping
Analysis perform the following sequence of operations. These steps
are not part of the V-2 rocket instructions but are directly
applicable.
1) On the main AeroCFD screen "click" the LOOP
icon to bring up the CFD Looping Analysis and Plots screen.
2) In the CFD Loop Analysis section select either AOA or
Velocity to perform a Loop Analysis of the plot variables
as a function of AOA or Velocity. For this example
select the AOA option button.
3) In the CFD Loop Analysis Data section insert the total
number of CFD Loops. Insert 21 CFD loops for this example.
4) In the CFD Loop Analysis Data section insert the Initial
AOA (DEGREES). This is the starting AOA performed by the Looping
Analysis. Insert 0.05 degrees for this example.
5) In the CFD Loop Analysis Data section insert the AOA
Increment (DEGREES). This is the amount the AOA is incremented
for each iteration of the CFD Loop Analysis. Insert 0.5475
degrees for this example.
6) Perform the CFD Looping Analysis by "clicking" the
plot icon in the CFD Looping Analysis section. The loop
counter is displayed to the right of the plot icon. The counter
indicates the progress of the CFD Looping Analysis. Finally, to
the right of the loop counter a Stop watch is provided to allow
the analysis to be interrupted or terminated.
7) "Click" back to main AeroCFD screen by "clicking"
the ninth icon on the toolbar.
Please remember that you need to "click" back using
the Return icon. Clicking the [X] box will kill the results
and delete the modifications.
NOTE: The Barrowman results may be plotted verses the Looping
Analysis results by clicking the second icon from the right. The
Barrowman results are plotted for standard body tube shapes and
are not plotted for Free-Form body tube shapes. Also, the Barrowman
results are not plotted for Velocity Loop Analyses. Finally,
a variety of options are provided at the toolbar, such as Send
formatted data to printer, Print screen, Save data
to disk, Increase Y-Axis scale, Reset Y-Axis,
and Plot Barrowman results.
CFD LOOPING ANALYSIS RESULTS DISCUSSION
The results plotted along with the CD and CN plots illustrated
below is an extension of the analysis presented on the AeroCFD
Description page. Please note the
excellent agreement between the modified Sutton data for drag
(CD) and normal force coefficient (CN) over the range between
0 to 12 degrees angle of attack. Because the Sutton data is in
the form of CD and CL a simple transformation of the data puts
the results into the form of CD and CN (CY). The following two
equations are solved simultaneously to determine CN (CY) in terms
of CD and CL. (1) CD = CY * sin(AOA) + CX * cos(AOA) and (2) CL
= CY * cos(AOA) - CX * sin(AOA) . The equation for CN (CY) is:
CN = [ CL + CD * tan (AOA) ] / [ cos(AOA) + sin (AOA) * tan (AOA)
] and is plotted along with the AeroCFD results and the Barrowman
equation results. The Modified Sutton data for drag (CD) do not
require a transformation and are shown plotted directly with the
AeroCFD results.
AeroCFD normal
force coefficient (CN) results exactly match modified Sutton V-2
CN data up to approximately 5 degrees angle of attack and then
begin to depart from the modified V-2 data. The departure between
the AeroCFD results for CN and the modified Sutton V-2 CN data
beyond 5 degrees is expected because AeroCFD does not model separation
effects as the gradients in the flow field become large and viscous
effects predominate. AeroCFD drag coefficient (CD) data track
the modified Sutton CD results over the entire range from 0.0
degrees to 12 degrees angle of attack. Also note the Barrowman
equation normal force coefficient (CN) predictions depart from
the AeroCFD and Modified Sutton results over the entire range
of the analysis. Therefore, this analysis indicates the Barrowman
CN results are not accurate at small AOA (0 to 5 degrees) for
boat tail shapes.
CD VERSES AOA LOOPING ANALYSIS
Please click the
ninth (Return) icon in the toolbar or click the CN option
button to view the CN plot.
CD verses AOA Loop Analysis
Display. Modified Sutton CD verses AOA plotted With AeroCFD Results
CN VERSES AOA LOOPING
ANALYSIS
Please click the
ninth (Return) icon in the toolbar or click the XCp option
button to view the XCp plot.
CN verses AOA Loop Analysis
Display. Modified Sutton CN verses AOA plotted With AeroCFD Results
AVERAGE CD
(DRAG) LOOPING ANALYSIS
This screen shot illustrates that AeroCFD will compute average
CD over a range of velocity. Click the Velocity option button
and define the total Number of Loops to be performed by AeroCFD.
Then, specify the constant angle of attack (Initial AOA), Initial
Rocket Flight Velocity (Normally from 1 to 5 ft/sec), and finally
the Rocket Velocity Increment that will provide the desired upper
limit on flight velocity. After the analysis is complete the Average
CD over the velocity range specified is displayed as illustrated
below. Use this value for drag coefficient (CD) in any flight
simulation computer program.

XCp VERSES AOA LOOPING ANALYSIS
Please click the
ninth (Return) icon in the toolbar.
XCp verses AOA Loop Analysis
Display
CROSS-FLOW DISTRIBUTION
The Cross-Flow pressure
Cp Distribution screen displays the pressure distribution
on the airframe at AOA. AeroCFD results are plotted verses the
potential flow equation of Cp verses angular location on the
body tube. For comparison with classical cross-flow results, the
AOA on the main screen of the analysis must be set to 90 degrees
for the results plotted here to agree with the potential flow
equation. For cross-flow comparisons, select a station well back
from the tip of the nose cone but before the base of the rocket.
These steps are not part of the V-2 rocket instructions.
Please click the fifth (Return) icon in the toolbar
(AOA = 90 degrees on main screen).
Cross-Flow Cp Distribution
Screen
FREE-FORM BODY TUBE
GEOMETRY
To use this screen perform
the following sequence of operations. These steps are not
part of the V-2 rocket instructions.
1) On the Body Tube Geometry screen click the Free-Form
Tube Geometry icon to bring up the free-form editor.
2) Select the total number of points that will describe the body
tube using the Points defining body up-down control. Select
up to 20 points that will define the body tube shape.
3) For better accuracy "click" the Resize icon
to maximize the plot area image. This will allow AeroCFD to use
all available pixels on your computer screen for more accuracy.
4) Using the cursor, drag each point into place one after the
other. Position each point by referencing the X-Location,
Y-Location and Y-Diameter values as they are updated
as you move the cursor.
5) "Click" back to the Body Tube Geometry screen
by "clicking" the eighth icon on the toolbar or the
large Return icon. Then "click" back to the main
AeroCFD screen.
Please remember that you need to "click" back using
the Return icon. Clicking the [X] box will kill the results
and delete the modifications.
Note: This screen does not represent the V-2 rocket example. It
is being provided for illustration and description. However, it
is part of a separate V-2 analysis that used a Free-Form body
tube instead of the Standard body tube geometry.
Please click the eighth (Return) icon in the toolbar
to return to the Body Tube Geometry screen.
V-2 Free-Form Geometry (Alternate
Method For generating Airframe Shape)
AERODYNAMIC
DEFINITIONS SECTION
1) Mach Number (Mn) = V / C, is the ratio of flow velocity (V)
at a point in the flow to the speed of sound (C) at that same
point in the flow.
2) Reynolds Number (Rn) = V L / v, is the ratio of dynamic forces
(Velocity * Length) to friction forces (Kinematic viscosity) at
a point in the flow.
3) Drag Coefficients (CD) = D / q S, is the drag force (D) in
the flow direction divided by the dynamic pressure (q) and the
reference area (S).
4) Lift Coefficient (CL) = L / q S, is the lift force (L) perpendicular
to the flow direction divided by the dynamic pressure (q) and
the reference area (S)
5) Drag Coefficients (CX) = X / q S, is the drag force (X) in
the axial direction of the rocket divided by the dynamic pressure
(q) and the reference area (S).
6) Lift Coefficient (CY) = Y / q S, is the lift force (Y) perpendicular
to the axial direction of the rocket divided by the dynamic pressure
(q) and the reference area (S).
7) Normal Force Coefficient (CN) = N / q S, is the normal force
(N) perpendicular to the axis of the rocket divided by the dynamic
pressure (q) and the reference area (S).
8) Pitch Moment Coefficient (CM) = M / q S L, is the pitch moment
(M) acting around the tip of the nose cone divided by the dynamic
pressure (q), reference area (S) and the reference length (L).
A negative pitch moment (CM) indicates that a positive angle of
attack will cause a restoring moment (M) tending to return the
rocket to equilibrium flight. Having a negative CM when AOA is
"positive" is a "good" thing. It means the
rocket is stable! In other words the rocket will try to
return to its stable equilibrium position (zero degrees AOA) when
a disturbance, like a gust of wind, acts on the rocket.
9) Rocket Cp location (Xcp) = XCp/L, is the non-dimensional location
of the center of pressure. XCp/L is computed by dividing the dimensional
location of the center of pressure (XCp) by the reference length
(L) of the rocket, normally the total rocket length. Center of
pressure is the location or point where the resultant of all distributed
aerodynamic loads effectively act on the body. Center of pressure
can also be computed from: XCp = - M / N, where the M acts around
the tip of the nose cone.
10) Rocket Base Drag Coefficient (Cd_Base) is the contribution
to pressure drag caused by the action of the insulating boundary
layer "jet-pump" on the surface of the rocket that tends
to "pump" air away from the base of the rocket causing
the static pressure at the base of the rocket to be reduced. Cd_base
= 0.029 / SQRT(Cfb) * (Dbase / Dbody)^3 . Where Cfb is the total
forebody drag coefficient that does not include base drag effects.
This relationship is valid for subsonic and supersonic flow. Cd_Base
ranges from 0.025 to 0.20 for most rockets. Note: For turbulent
boundary layer flow the forebody drag coefficient (Cfb) can be
estimated to be a function of Mach number, Reynolds number and
body shape.
11) Dynamic Pressure (q) = 1/2 * Air Density * V^2.
12) CD, CL, CX and CY are related by the equations: CD = CY *
sin(AOA) + CX * COS(AOA) and CL = CY * COS(AOA) - CX * SIN(AOA).
13) Static Pressure = Total Pressure - Dynamic Pressure. Can be
understood to be the pressure between streamlines in the flow.
14) Total Pressure = Pressure that would exist in a flow if the
flow were slowed isentropically to zero velocity. Also called
stagnation pressure for subsonic flow.
15) Dynamic Pressure = 1/2 * Air Density * V^2.
16) Pressure Coefficient (Cp) = (P - PINF) / q. Definition of
pressure coefficient. Where P is the pressure anywhere in the
flow, PINF is the freestream pressure and q is the dynamic pressure.
17) Derivative of Normal Force Coefficient (CNa) is the slope
of CN verses angle of attack . Specifically, CNa = (CN1 - CN2)
/ (AOA1 - AOA2).
NOTE: For more discussion on these topics please read Fluid
Dynamic Drag, by S.F. Hoerner. This is an excellent book and
is easy to understand.
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AeroCFD® 2D-WING Bonus Feature Addition, Instructions BACK |
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AeroCFD includes a new program called 2D-WING™ for the aerodynamic analysis of two-dimensional (2-D) and finite aspect ratio (AR) airfoil sections. 2D-WING uses vortex lift panels to compute CD, CL and Cm,c/4 for airfoil sections using NACA four digit airfoils, streamlined, flat plate, double wedge (D'Wedge) and imported custom shapes for a wide range of 2-D and finite AR airfoils. Several NACA five-digit airfoils from Appendix III in the book Theory of Wing Sections allow the user to rapidly specify complex imported shapes. Other useful input variables include wing Reynolds number (Re) and angle of attack in degrees. Also, 2D-WING produces filled color contour plots and line color contour plots for pressure coefficient (Cp) and U/U0 where the number of contour levels can be specified from 3 to 256 levels. In addition, the following standard plots are produced, Cp verses chord length and U/U0 verses chord length for the upper and lower airfoil surfaces. Also, CL verses AOA, CD verses AOA, CD verses CL, CL/CD verses AOA and Cm verses AOA are quickly plotted. Finally, the total number of 2-D vortex panels that define the upper and lower surfaces of an airfoil can be specified as 100, 200 or 300. |
AeroCFD 2D-WING uses 2D vortex lift panels
to determine drag coefficient (CD), lift coefficient (CL) and moment coefficient
(Cm,c/4) of airfoil sections. Airfoil section shapes are specified using the NACA four digit series, Streamlined, Flat
Plate, D'Wedge and Imported shape options. The following steps outline the
basic procedure used to operate AeroCFD 2D-WING.
Step 1. The
specification of Streamlined, Flat Plate and D'Wedge airfoil section shapes
requires the specification of fin thickness in terms of maximum thickness in percent
chord (Tmax/Chord X 100). Maximum fin thickness in percent chord for all airfoil
types is specified by using the third data entry box on the
first line, NACA Four-Digit
series airfoil description. The first two data entry boxes for Streamlined,
Flat Plate and D'Wedge airfoil section shapes are disabled. However, for the NACA
Four-Digit series, the first two data entry boxes are enabled, where the first
data entry box refers to maximum camber in percent chord and the second data
entry box refers to position of the maximum camber in tenths of a chord from the
leading edge (LE).
The following definitions are needed to define camber and camber location for
NACA airfoils. First, the mean camber line is the locus of points halfway
between the upper and lower surfaces of the airfoil as measured perpendicular to the mean
camber line. Then, the chord line is a straight line that connects the leading and
trailing edges of the airfoil and is simply referred to as the chord of the
airfoil and is usually defined using the symbol, c. Using these definitions the
camber is the maximum perpendicular distance between the mean camber line and
the chord line of the airfoil. Camber location is simply located as a percentage
of the chord length from the leading edge of the airfoil.
The complete specification of four-digit NACA airfoils and standard airfoils are
summarized below for the first line, NACA Four-Digit
series airfoil description. Where the first two spaces are disabled for
Streamlined, Flat Plate, and D'Wedge airfoil section shapes but are required for
NACA four-Digit airfoils.
[Max camber in percent chord], [Position of max camber in
1/10th chord],
[Max thickness in percent chord].
Step 2. The Reynolds number (Re =
rUc/m)
of the fin is defined on the second line of input data. Reynolds number is
defined as the ratio of the inertial forces represented by the density of
the medium (r),
free stream velocity (U), and fin dimension (c) to the friction forces in
the boundary layer represented by the viscosity of the medium (m).
Reynolds number is automatically inserted if entering from AeroCFD Rocket
but is an input if entering from the AeroCFD 2D-WING command buttons. The
following
Reynolds
number calculator is useful for computing Reynolds number for AeroCFD 2D-WING (Note:
This off-site calculator has not been checked for accuracy). For
more information and theory about Reynolds number please visit the
Wikipedia on-line
encyclopedia.
Step 3. Fin angle of attack (a)
is defined relative to the chord line for all section shapes on the third line
of input data.
Step 4. Fin aspect ratio (AR = Span/Chord) is defined on the fourth line
of input data. Aspect ratio must be non-zero and Checked to be included
in the computation of CD, CL and Cm,c/4. The Aspect ratio input allows an
"approximate solution" of end effects and 3D wings.
Step 5. Select one of five fin section shapes using the Airfoil Shapes
pull-down menu. Streamlined, NACA four-digit, Flat Plate
and D'Wedge section shapes are directly drawn after selection. In
addition, arbitrary fin section shapes may be defined using the Import X-Y
command. Many NACA Five-Digit section shapes are included in
NACA_AIRFOILS.zip (located in the AeroCFD directory) and are drawn by
using the Import X-Y command after unzipping the file.
Import File format for each station (X) and ordinate (Y) given in percent
of airfoil chord (LE is the Leading Edge): [Upper Surface X-location from LE],
[Upper Surface Y-location from Chord Line], [Lower
Surface X-location from LE], [Lower Surface Y-location from Chord
Line]
for each station from the LE to TE.
Step 6. Perform a 2D Vortex Panel aerodynamics analysis by
clicking the SOLVE command button and follow the instructions
displayed in the lower left status bar. Instructions displayed in the Status bar
will state when a valid solution is achieved and when it is permissible to click
the various plot command buttons.
Step 7. Display results using the following commands in the Plots
pull-down menu: Cp verses X, U/U0 verses X, CL verses AOA, CD verses AOA, CD
verses CL, CL/CD verses AOA, Cm verses AOA, U/U0 Contours (Filled and Line) and
finally Cp Contours (Filled and Line). Where AOA refers to angle of attack in
degrees, Cp = (P - PINF) / q = 1 - (U/U0)^2 is the pressure coefficient and U0
refers to the free stream velocity. Please note the results obtained by
modifying data in AeroCFD 2D-WING are not reflected back into the AeroCFD
Rocket analysis except for the number of panels that define the airfoil
section. However, fin shapes used on the Fin and Launch Lug Geometry
screen may be analyzed and the results plotted in AeroCFD 2D-WING. Reference:
THEORY OF WING SECTIONS, by Abbott and Doenhoff.

Figure 1, Fin Vortex Panel Method Analysis
Screen, U/U0 Filled Contours and U/U0 verses X.

Figure 2, Fin Vortex Panel Method Analysis
Screen, Cp (pressure coefficient) Line Contours and Cp verses X.
(1)
NACA 0012 AIRFOIL VALIDATION
Figure 3, NACA 0012 CL verses AOA and CD verses CL.
(2) NACA 63-212 AIRFOIL VALIDATION
Figure 4, NACA 63-212 CL verses AOA and CD verses CL.
NOTES:
1) Reference: THEORY OF WING SECTIONS,
by Abbott
and Doenhoff.
2) AeroCFD 2D-WING results (red dots)
generated using the Save Results As command under File. The
Results were plotted using Excel (or any spreadsheet program) and compared to THEORY OF
WING SECTIONS data for the NACA 0012 and NACA 63-212 wing sections.
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