AERODYNAMIC
ANALYSIS
OF
THE
CARBON
DRAGON AIRFOILS
About the author:
Alejandro Ramirez-Pineiro (30) has the degree of
Bachelor of Science in Mechanical Engineering, earned at the Universidad
Tecnologica Metropolitana of Santiago, Chile. At this moments he is working as
a Composite Materials Engineer at ENAER, building a 100% composite JAR 23
airplane (visit www.euro-enaer.com ).
Also he is building a modified Carbon Dragon, planned to fly during the first
quarter of 2000. You can reach him at alejo@netline.cl
.
Introduction:
The Carbon Dragon is an ultralight, high
performance glider. This glider was conceived by Jim Maupin who also
designed the famous Woodstock sailplane and the Windrose motorglider.
With encouragement from Irv Culver, who promised to "run the
numbers", Jim Maupin finished the design and built the prototype. As
a result, Jim Maupin with an assist from co-designer Irv Culver, produced an exciting
sailplane.
Scope of the study:
The proposal of this study is getting aerodynamic data
that can be used for the structural modifications of the original Carbon
Dragon. This data will be used also
on the study of the longitudinal static
stability of the modified glider. All the aerodynamic values presented here can
be useful to actual or future builders for helping their own studies.
For preliminary design,
the values presented in this report are excelent, but must to keep in mind that
the data presented here was developed by a computer software, so, to get more
“real” values, the reader will have to do wind tunnel testing.
Getting the coordinates:
To get the coordinates
of the wing root and wing tip airfoils, the original drawings of the ribs
number 1 and number 13 where divided on 88 stations on the root and 58 stations
on the tip. The mesures where taken with an accuracy of + - 0.5 mm. The job was done by my building
partner Miguel Eyquem.
With the coordinates
obtained in milimiters, the next step was to convert them in fractions of
chord. For this task I used an electronic spreadsheet.
(values on fraction of chord)
|
Coord |
x |
Yu |
Yl |
|
Coord |
X |
Yu |
Yl |
|
0 |
0 |
0 |
0 |
|
51 |
0.361367 |
0.116951 |
-0.07819 |
|
1 |
0.001314 |
0.00657 |
-0.00591 |
|
52 |
0.374507 |
0.115966 |
-0.07819 |
|
2 |
0.003285 |
0.010184 |
-0.00828 |
|
53 |
0.387648 |
0.114652 |
-0.07806 |
|
3 |
0.00657 |
0.014783 |
-0.0115 |
|
54 |
0.400788 |
0.113338 |
-0.07779 |
|
4 |
0.009855 |
0.018725 |
-0.0138 |
|
55 |
0.413929 |
0.111695 |
-0.0772 |
|
5 |
0.013141 |
0.022339 |
-0.01577 |
|
56 |
0.42707 |
0.110381 |
-0.07668 |
|
6 |
0.016426 |
0.026281 |
-0.01774 |
|
57 |
0.44021 |
0.108541 |
-0.07615 |
|
7 |
0.019711 |
0.029566 |
-0.01971 |
|
58 |
0.453351 |
0.106767 |
-0.0753 |
|
8 |
0.022996 |
0.032852 |
-0.02102 |
|
59 |
0.466491 |
0.105125 |
-0.07424 |
|
9 |
0.026281 |
0.035808 |
-0.02234 |
|
60 |
0.479632 |
0.103154 |
-0.07326 |
|
10 |
0.029566 |
0.038765 |
-0.02431 |
|
61 |
0.492773 |
0.101183 |
-0.07194 |
|
11 |
0.032852 |
0.041393 |
-0.02562 |
|
62 |
0.505913 |
0.099212 |
-0.0707 |
|
12 |
0.036137 |
0.044678 |
-0.02727 |
|
63 |
0.519054 |
0.096912 |
-0.06932 |
|
13 |
0.039422 |
0.047306 |
-0.02858 |
|
64 |
0.532194 |
0.094941 |
-0.06754 |
|
14 |
0.042707 |
0.049934 |
-0.02989 |
|
65 |
0.545335 |
0.092576 |
-0.06597 |
|
15 |
0.045992 |
0.052562 |
-0.03121 |
|
66 |
0.565046 |
0.08883 |
-0.06334 |
|
16 |
0.049277 |
0.054534 |
-0.03252 |
|
67 |
0.584757 |
0.085414 |
-0.06064 |
|
17 |
0.052562 |
0.056505 |
-0.03351 |
|
68 |
0.604468 |
0.08134 |
-0.05782 |
|
18 |
0.055848 |
0.059133 |
-0.03463 |
|
69 |
0.624179 |
0.076938 |
-0.05519 |
|
19 |
0.059133 |
0.061104 |
-0.03581 |
|
70 |
0.64389 |
0.07293 |
-0.05256 |
|
20 |
0.062418 |
0.063403 |
-0.03679 |
|
71 |
0.663601 |
0.06866 |
-0.04961 |
|
21 |
0.065703 |
0.065703 |
-0.03784 |
|
72 |
0.683311 |
0.064389 |
-0.04652 |
|
22 |
0.072273 |
0.068988 |
-0.04008 |
|
73 |
0.703022 |
0.05979 |
-0.04336 |
|
23 |
0.078844 |
0.072273 |
-0.04172 |
|
74 |
0.722733 |
0.055191 |
-0.04074 |
|
24 |
0.085414 |
0.075558 |
-0.04382 |
|
75 |
0.742444 |
0.050591 |
-0.03752 |
|
25 |
0.091984 |
0.078844 |
-0.04534 |
|
76 |
0.762155 |
0.047306 |
-0.03476 |
|
26 |
0.098555 |
0.0818 |
-0.04731 |
|
77 |
0.781866 |
0.043364 |
-0.03187 |
|
27 |
0.105125 |
0.084757 |
-0.04901 |
|
78 |
0.801577 |
0.039093 |
-0.02891 |
|
28 |
0.111695 |
0.087385 |
-0.05099 |
|
79 |
0.821288 |
0.035085 |
-0.02602 |
|
29 |
0.118265 |
0.090013 |
-0.05256 |
|
80 |
0.840999 |
0.031012 |
-0.023 |
|
30 |
0.124836 |
0.092313 |
-0.05414 |
|
81 |
0.86071 |
0.026938 |
-0.0203 |
|
31 |
0.131406 |
0.094415 |
-0.05565 |
|
82 |
0.88042 |
0.022996 |
-0.01537 |
|
32 |
0.137976 |
0.096583 |
-0.05696 |
|
83 |
0.900131 |
0.018922 |
-0.01445 |
|
33 |
0.144547 |
0.098555 |
-0.05848 |
|
84 |
0.919842 |
0.01498 |
-0.0113 |
|
34 |
0.151117 |
0.100657 |
-0.05999 |
|
85 |
0.939553 |
0.010841 |
-0.00821 |
|
35 |
0.157687 |
0.102497 |
-0.0611 |
|
86 |
0.959264 |
0.006899 |
-0.00512 |
|
36 |
0.164258 |
0.104205 |
-0.06242 |
|
87 |
0.978975 |
0.002957 |
-0.0021 |
|
37 |
0.177398 |
0.107753 |
-0.06472 |
|
88 |
1 |
0 |
0 |
|
38 |
0.190539 |
0.11071 |
-0.06669 |
|
|
|
|
|
|
39 |
0.203679 |
0.113009 |
-0.06866 |
|
|
|
|
|
|
40 |
0.21682 |
0.115375 |
-0.07063 |
|
|
|
|
|
|
41 |
0.229961 |
0.116754 |
-0.07194 |
|
|
|
|
|
|
42 |
0.243101 |
0.118265 |
-0.07293 |
|
|
|
|
|
|
43 |
0.256242 |
0.119054 |
-0.07392 |
|
|
|
|
|
|
44 |
0.269382 |
0.119842 |
-0.0749 |
|
|
|
|
|
|
45 |
0.282523 |
0.119908 |
-0.07589 |
|
|
|
|
|
|
46 |
0.295664 |
0.11958 |
-0.07654 |
|
|
|
|
|
|
47 |
0.308804 |
0.119251 |
-0.07727 |
|
|
|
|
|
|
48 |
0.321945 |
0.119054 |
-0.07753 |
|
|
|
|
|
|
49 |
0.335085 |
0.118594 |
-0.07786 |
|
|
|
|
|
|
50 |
0.348226 |
0.117937 |
-0.07819 |
|
|
|
|
|

(values on fraction of chord)
|
Coord |
X |
Yu |
Yl |
|
Coord |
X |
Yu |
Yl |
|
0 |
0 |
0 |
0 |
|
31 |
0.363278 |
0.100036 |
-0.0349 |
|
1 |
0.00179 |
0.011632 |
-0.01163 |
|
32 |
0.381174 |
0.098425 |
-0.03364 |
|
2 |
0.005369 |
0.020401 |
-0.01825 |
|
33 |
0.399069 |
0.096994 |
-0.03239 |
|
3 |
0.010737 |
0.027738 |
-0.02523 |
|
34 |
0.416965 |
0.095204 |
-0.03185 |
|
4 |
0.017895 |
0.034896 |
-0.03114 |
|
35 |
0.43486 |
0.093057 |
-0.03042 |
|
5 |
0.025054 |
0.040444 |
-0.0349 |
|
36 |
0.452756 |
0.091267 |
-0.02953 |
|
6 |
0.032212 |
0.046528 |
-0.03758 |
|
37 |
0.470651 |
0.089298 |
-0.02845 |
|
7 |
0.03937 |
0.051897 |
-0.03937 |
|
38 |
0.488547 |
0.086793 |
-0.02756 |
|
8 |
0.048318 |
0.057266 |
-0.04116 |
|
39 |
0.506442 |
0.084109 |
-0.02649 |
|
9 |
0.057266 |
0.063529 |
-0.04295 |
|
40 |
0.524338 |
0.081424 |
-0.02523 |
|
10 |
0.066213 |
0.068003 |
-0.04384 |
|
41 |
0.542233 |
0.07874 |
-0.02416 |
|
11 |
0.075161 |
0.072656 |
-0.04474 |
|
42 |
0.560129 |
0.077666 |
-0.02309 |
|
12 |
0.085898 |
0.076951 |
-0.04545 |
|
43 |
0.578024 |
0.072656 |
-0.02219 |
|
13 |
0.094846 |
0.08053 |
-0.04563 |
|
44 |
0.59592 |
0.069792 |
-0.02112 |
|
14 |
0.103794 |
0.083751 |
-0.04581 |
|
45 |
0.613815 |
0.066571 |
-0.02004 |
|
15 |
0.112742 |
0.086256 |
-0.04563 |
|
46 |
0.631711 |
0.063529 |
-0.01915 |
|
16 |
0.121689 |
0.089298 |
-0.04617 |
|
47 |
0.649606 |
0.060845 |
-0.0179 |
|
17 |
0.130637 |
0.091267 |
-0.04635 |
|
48 |
0.667502 |
0.057266 |
-0.01646 |
|
18 |
0.139585 |
0.093057 |
-0.04653 |
|
49 |
0.685397 |
0.054581 |
-0.01611 |
|
19 |
0.148533 |
0.094846 |
-0.04635 |
|
50 |
0.721188 |
0.048318 |
-0.01432 |
|
20 |
0.166428 |
0.098067 |
-0.04384 |
|
51 |
0.756979 |
0.041696 |
-0.01217 |
|
21 |
0.184324 |
0.100215 |
-0.04295 |
|
52 |
0.79277 |
0.035791 |
-0.01056 |
|
22 |
0.202219 |
0.101467 |
-0.04259 |
|
53 |
0.828561 |
0.029707 |
-0.00823 |
|
23 |
0.220115 |
0.102362 |
-0.0417 |
|
54 |
0.864352 |
0.023264 |
-0.00626 |
|
24 |
0.23801 |
0.103078 |
-0.0408 |
|
55 |
0.900143 |
0.01718 |
-0.00447 |
|
25 |
0.255906 |
0.103615 |
-0.03991 |
|
56 |
0.935934 |
0.010916 |
-0.00268 |
|
26 |
0.273801 |
0.103794 |
-0.03919 |
|
57 |
0.971725 |
0.004295 |
-0.00089 |
|
27 |
0.291696 |
0.103794 |
-0.03812 |
|
58 |
1 |
0 |
0 |
|
28 |
0.309592 |
0.102899 |
-0.0374 |
|
|
|
|
|
|
29 |
0.327487 |
0.102004 |
-0.03669 |
|
|
|
|
|
|
30 |
0.345383 |
0.10111 |
-0.03579 |
|
|
|
|
|

Image 2. Carbon Dragon Wing Tip Airfoil.
Using the software:
The software used was Airfoil
Analysis Geometric Module (to get more information and/or demos visit http://airfanalysis.hypermart.net ) developed by two Engineers
at Italy.
The data was imported
from a text file into the Coorditate Editor to make easier the data imput to
the software.
Using both airfoils (root and tip) was possible to get by interpolation the mean geometric chord airfoil, slightly different from the Mean Aerodynamic Chord, for a simply, linearly tapered wing. For this task I used the Airfoil Mix Window and set the mix proportion to 50 %. See the Mean Geometric Chord coordinates table.
With the coordinates of
the root, tip and Mean Geometric Chord airfoils the software was able to give
the following information:
1.- Geometric data of
the airfoils
2.- Estimated
aerodynamic data, including:
·
Angle of atack for zero lift, a 0
·
Pitching moment at zero lift, Cm0
·
Lift slope, a0
(values on fraction of chord)
|
Coord |
x |
Yu |
Yl |
|
0 |
0 |
0 |
0 |
|
1 |
0.0016 |
0.0092 |
-0.0087 |
|
2 |
0.0065 |
0.0184 |
-0.0156 |
|
3 |
0.0145 |
0.028 |
-0.0227 |
|
4 |
0.0257 |
0.0381 |
-0.0286 |
|
5 |
0.04 |
0.05 |
-0.0342 |
|
6 |
0.0573 |
0.0618 |
-0.039 |
|
7 |
0.0774 |
0.0726 |
-0.0431 |
|
8 |
0.1003 |
0.0826 |
-0.0468 |
|
9 |
0.1257 |
0.0915 |
-0.0503 |
|
10 |
0.1536 |
0.0986 |
-0.0531 |
|
11 |
0.1838 |
0.1047 |
-0.0543 |
|
12 |
0.216 |
0.1087 |
-0.0562 |
|
13 |
0.25 |
0.1111 |
-0.0568 |
|
14 |
0.2857 |
0.1119 |
-0.0573 |
|
15 |
0.3227 |
0.1107 |
-0.0572 |
|
16 |
0.3609 |
0.1086 |
-0.0566 |
|
17 |
0.4 |
0.1052 |
-0.0551 |
|
18 |
0.4397 |
0.1006 |
-0.0531 |
|
19 |
0.4799 |
0.0956 |
-0.0507 |
|
20 |
0.5201 |
0.0894 |
-0.0473 |
|
21 |
0.5603 |
0.0837 |
-0.0435 |
|
22 |
0.6 |
0.0757 |
-0.0396 |
|
23 |
0.6391 |
0.0681 |
-0.036 |
|
24 |
0.6773 |
0.0607 |
-0.0318 |
|
25 |
0.7143 |
0.0534 |
-0.0283 |
|
26 |
0.75 |
0.0461 |
-0.0245 |
|
27 |
0.784 |
0.0401 |
-0.0213 |
|
28 |
0.8162 |
0.034 |
-0.0179 |
|
29 |
0.8464 |
0.0282 |
-0.0148 |
|
30 |
0.8743 |
0.0229 |
-0.0113 |
|
31 |
0.8997 |
0.0181 |
-0.0095 |
|
32 |
0.9226 |
0.0138 |
-0.0071 |
|
33 |
0.9427 |
0.0099 |
-0.005 |
|
34 |
0.96 |
0.0066 |
-0.0032 |
|
35 |
0.9743 |
0.0039 |
-0.0018 |
|
36 |
0.9855 |
0.0019 |
-0.0008 |
|
37 |
0.9935 |
0.0007 |
-0.0003 |
|
38 |
0.9984 |
0.0002 |
0 |
|
39 |
1 |
0 |
0 |

Image 3. Carbon Dragon Mean Geometric Chord.
|
|
Wing
root airfoil |
Mean
Geometric Chord airfoil |
Wing
tip airfoil |
|
Maximum thickness |
19.67 % |
16.91 % |
14.42 % |
|
Position max. thickness |
31.30 % |
28.43 % |
20.87 % |
|
Maximum camber |
2.27 % |
2.74 % |
3.29 % |
|
Position max. camber |
24.55 % |
27.30 % |
29.57 % |
|
Leading edge radius |
0.68 % |
1.67 % |
2.19 % |
|
Trailing edge angle |
17.23 degrees |
14.44 degrees |
11.63 degrees |
|
Geometric centroid in X |
41.43 % |
40.12 % |
38.34 % |
|
Geometric centroid in Y |
1.56 % |
2.05 % |
2.49 % |
|
|
Wing
root airfoil |
Mean
Geometric Chord airfoil |
Wing
tip airfoil |
|
a 0 [degrees] |
-1.27 |
-1.92 |
-2.57 |
|
Cm0 |
-0.0158 |
-0.0357 |
-0.0557 |
|
Lift
curve slope efficiency factor m |
1.0153 |
1.0132 |
1.0112 |
|
Lift
slope, a0 [1/degree] |
0.111 |
0.111 |
0.110 |
Observations
regarding the geometric characteristics of the airfoils:
a) The increasing camber toward the tip should be due
to a research of higher maximum lift coefficients to avoid tip stalling.
b)
Progressively moving forward the maximum center position should be due to
obtain earlier transition on the tip section and minimize Reynolds number
effects.
c)
The increase of the L.E. radius help to soften tip stall.
For the eager builder/designer:
Some remarks about the “estimated” aerodynamic data
presented in AIRFOIL ANALYSIS – GEOMETRIC MODULE: The estimates of zero lift
angle and zero lift quarter chord moment coefficient are obtained by the
Pankurst’s method (“Theory of Wing Sections”,
by Abbott and von Doenhoff) … relying just upon the knowledge of the mean line
shape: it’s a sort of Gaussian quadrature and it should had been developed
analytically, so no numeric is still present at this stage. The method is
surprisingly good, relating to its simplicity, as you own will experience when
comparing estimated to calculated data (by the numerical panel method or
comparison with experiments). In fact, the flow quality on the airfoil surfaces
is still “good” in the proximity of the zero lift angle (that is usually small)
for conventional, unflapped airfoils … this explains why these estimates are
incredibly useful even if absolutely “a priori” of any aerodynamic analysis as
properly defined.
The lift curve slope efficiency factor m (the ratio of the potential flow slope to the theoretical value of 2p) is estimated according to R. Eppler (“Airfoil Design and Data”, Springer Verlag) but it’s usefulness is
usually driven off by viscous effects … so practically it doesn’t matter
anymore when viscous analysis are on hand.
References:
http://airfanalysis.hypermart.net
http://airfanalysis.hypermart.net
http://www.isd.net/sadkins/builders.htm
Jim
Maupin Ltd.
www.jcpress.com/JMaupinLtd/carbon.htm
The part II of this
study will include: