Parasite drag is a combination of form, friction, and interference drag that is evident in any body moving through a fluid. Although VSPAERO includes an estimate of parasite drag in the calculation of the zero lift drag coefficient, the Parasite Drag tool provides much more advanced options and capabilities. The Parasite Drag Tool GUI is accessed by clicking “Parasite Drag…” from the Analysis drop-down on the top menu-bar.

$ c_i \equiv \mbox{Chord length at span station} $
$ b_i \equiv \mbox{Section span} $
$ S_i \equiv \mbox{Section area} $
$ S_{total} \equiv \mbox{Total Area} $
$ \bar{c} \equiv \mbox{Weighted chord sum} $
$ L_{ref} \equiv \mbox{Reference length} $
$ D \equiv \mbox{Diameter} $
$ X_{area} \equiv \mbox{Max cross sectional area} $
$ FR \equiv \mbox{Fineness ratio} $
$ Re \equiv \mbox{Reynolds number} $
$ V_{inf} \equiv \mbox{freestream velocity} $
$ \nu \equiv \mbox{kinematic viscosity} $
$ C_{f} \equiv \mbox{friction coefficient} $
$ f \equiv \mbox{flat plate drag} $
$ S_{wet} \equiv \mbox{wetted area} $
$ S_{ref} \equiv \mbox{reference area} $
$ C_D \equiv \mbox{coefficient of drag} $

Visible on all tabs of the GUI is the parasite drag table, which identifies individual components and their inputs in the parasite drag calculation. The table may be sorted by Component, S_wet, or % Total by selecting the toggles at the top of the table. Clicking on a geometry in the Component column of the table will break up the geometry into its surfaces and sub-surfaces. Below the list of components, excrescences are identifies, for which the Excrescence tab is available to add, remove, and adjust excrescences. Once the table has been setup, the “Calculate CDO” button on the bottom left of the GUI will run the parasite drag calculation. Once finished, the results will update in real time in response to changes in input values, such as the flow condition. However, if a component is added, removed, or modified, the tool must be rerun. The entire Parasite Drag table, excrescence list, and total results can be exported by selecting “Export to *.csv”. Next to this button, the Export Sub-Components toggle is available to include or ignore component breakup in the export file. On the bottom right of the GUI, the total form factor, drag coefficient, and percent contribution to total drag is listed for all components, excrescences, and the combination of both.

Wetted areas for all components are taken from executing Comp Geom for the indicated geometry set and as such as are appropriately trimmed.

Utilizing this feature the user is able to combine the wetted area of any geometry with that of another. Currently, geometries can only be grouped with their ancestors and geometries of the same shape type.

This can be used for example if the gear pod is modeled seperately from the fuselage but the wetted area of the gear pod should be applied with the drag qualities (e.g. length, form factor, etc.) of the fuselage.

By default, subsurfaces are incorporated as a part of the geometry as a whole. In other words, the surfaces do not subtract any wetted area from the geometry or have any of their own unique properties. However, the parasite drag tool let's the user choose these as options if they desire.

The three options are:

• Treat as Parent
• Separate Treatment
• Zero Drag

Treat as Parent: The default option, incorporates the wetted area of the subsurface as part of a continuous geometry.

Separate Treatment: Allows the user, to some extent, control the qualities of the subsurface. However, due to limitations of the methodology used, the geometry based qualities (e.g. L_{ref}, Re, etc.) are derived from the parent geometry. The user is allowed to change the form factor equation type, manually set the laminar percentage, and manually set the interference factor for the subsurface.

Zero Drag:The subsurface wetted area is subtracted from the total wetted area of the geometry and no longer contributes to the drag of the component.

Reference length is calculated according to it's geometry type internal to VSP; either a “Wing” type or a “Body” type. If the result of these calculations are zero, due to rotation or abnormal geometry shape the other equation is attempted as a fail safe. If neither of these methods yield a result greater than zero, a default value of 1.0 is used as to prevent division by zero when calculating fineness ratio.

Wing reference length is found by taking the area weighted chord.

First find the width of the wing section. $$ \Delta_x = |x_{le(1)} - x_{le(end)}| $$ $$ \Delta_y = |y_{le(1)} - y_{le(end)}| $$ $$ \Delta_z = |z_{le(1)} - z_{le(end)}| $$ $$ b_i = \sqrt{ {\Delta_x}^2 + {\Delta_y}^2 + {\Delta_z}^2} $$ $$ S_i = b_i * \frac{c_i + c_{\left(i+1\right)}}{2} $$ $$ S_{total} = \sum\left(S_i\right) $$ $$ \bar{c} = \sum\left(\frac{c_i + c_{\left(i+1\right)}}{2}\right) $$ $$ L_{ref} = \frac{\bar{c}}{S_{total}} $$

Body geometry reference lengths are calculated by taking the distance between to the front and back ends of the degenerated stick. $$ \Delta_x = |x_{le(1)} - x_{le(end)}| $$ $$ \Delta_y = |y_{le(1)} - y_{le(end)}| $$ $$ \Delta_z = |z_{le(1)} - z_{le(end)}| $$ $$ L_{ref} = \sqrt{ {\Delta_x}^2 + {\Delta_y}^2 + {\Delta_z}^2} $$

Thickness to chord takes the max thickness to chord from the degenerate stick created from Degen Geom.

Fineness Ratio is calculated by taking the diameter calculated using the max cross sectional area taken from the degenerate stick from Degen Geom.

$$ D = 2 * \sqrt{\frac{X_{area}}{\pi}} $$ $$ F = \frac{D}{L_{ref}} $$

Depending on the atmosphere input type, the kinematic viscosity is calculated accordingly and used to find the Reynolds number for the geometry.

$$ Re = \frac{V_{inf} * L_{ref}}{\nu} $$

Laminar Percent takes a 0 to 100 value and at default is set to 0% for a fully turbulent flow.According to Raymer, most aircraft have 10-20% laminar flow over lifting surfaces, and almost no laminar flow over the fuselage. However, an aircraft like the Piaggio GP180 can have up to 50% laminar flow over the wings and tail and 20-35% over the fuselage$^{22}$.

The laminar friction coefficient is calculated using the following equation: $$ C_f = C_{f (100\%Turb)} - \left(C_{f (\% Partial Turb)} * \% Lam\right) + \left(C_{f (\% Partial Lam)} * \% Lam\right) $$

where (using a chosen friction coefficient and it's corresponding inputs) $$ C_{f (\% Partial Turb)} = f\left(Re_{Lam}\right) $$ $$ C_{f (\% Partial Lam)} = f\left(Re_{Lam}\right) $$ where $$ Re_{Lam} = Re * \% Lam $$

$ Q \equiv \mbox{Scale factor applied to drag coefficient} $

$$ f = S_{wet} * Q * C_f * FF $$

$$ C_D = \frac{f}{S_{ref}} $$

Unfortunately, there is substantial opportunity for confusion around the equations for the skin friction coefficient. The primary source of confusion is inconsistent nomenclature in the literature around two related quantities – the local skin friction coefficient vs. the flat plate average skin coefficient. Different references use inconsistent nomenclature to differentiate these quantities. A reader must be pedantic to verify that they understand the notation for any given publication. Often, the nomenclature is defined far away from where the equations are presented.

This analysis is only concerned with the flat plate average skin friction coefficient, which will be denoted $C_f$ herein.

$ x \equiv \mbox{distance along chord} $
$ k \equiv \mbox{roughness height} $
$ \gamma \equiv \mbox{specific heat ratio} $
$ r \equiv \mbox{recovery factor} = 0.89 $
$ n \equiv \mbox{viscosity power-law exponent} = 0.67 $

$ l \equiv \mbox{length of component} $
$ d \equiv \mbox{diameter of component} $
$ w \equiv \mbox{width at maximum cross sectional area} $
$ h \equiv \mbox{height at maximum cross sectional area} $
$ FR \equiv \mbox{Covert Fineness Ratio} = \frac{l}{\sqrt{wh}} $
$ l_{r} \equiv \mbox{Length of Fuselage} $
$ A_{x} \equiv \mbox{Cross Sectional Area of Fuselage} $
$ Q \equiv \mbox{Interference Factor} $

$$ C_f = \frac{1.32824}{\sqrt{Re}}\ $$

$$ C_f = \frac{0.455}{\ln^2(0.06\ Re)}\ $$

$$ C_f = \frac{0.430}{\log(Re)^{2.32}}\ $$

$$ \frac{1}{\sqrt{C_f}}\ = 3.46\log\left(Re\right) - 5.6 $$

$$ \log\left(Re\ C_f\right) = \frac{0.242}{\sqrt{C_f}}\ $$

$$ \frac{1}{\sqrt{C_f}}\ = 4.13\log\left(Re\ C_f\right) $$

$$ C_f = \frac{0.072}{Re^{1/5}}\ $$

$$ C_f = \frac{0.074}{Re^{1/5}}\ $$

$$ C_f = \frac{0.0315}{Re^{1/7}}\ $$

$$ C_f = \frac{0.0725}{Re^{1/5}}\ $$

$$ C_f = \frac{0.455}{\log\left(Re\right)^{2.58}}\ $$

$$ C_f = \frac{0.427}{\left(\log\left(Re\right) - 0.407\right)^{2.64}}\ $$

$$ C_f = \left(1.89 + 1.62\ \log\left(\frac{l}{k}\right)\right)^{-2.5} $$

$$ C_f = \frac{\left(1.89 + 1.62\ \log\left(\frac{l}{k}\right)\right)^{-2.5}}{\left(1 + \frac{\gamma - 1}{2}\ M_\infty\right)^{0.467}} $$

$$ f = \frac{\left(1 + 0.22\ r\ \frac{\gamma - 1}{2}\ {M_e}^2\ \frac{Te}{Tw}\right)}{\left(1 + 0.3\ \left(\frac{Taw}{Tw} - 1\right)\right)} $$ $$ C_f = \frac{0.451\ f^2\ \frac{Te}{Tw}}{\ln^2\left(0.056\ f\ \frac{Te}{Tw}^{1+n}\ Re\right)} $$

$$ FF = 1 + \frac{t}{c}\ \left(2.94206 + \frac{t}{c}\ \left(7.16974 + \frac{t}{c}\ \left(48.8876 + \frac{t}{c}\ \left(-1403.02 + \frac{t}{c}\ \left(8598.76 + \frac{t}{c}\ \left(-15834.3\right)\right)\right)\right)\right)\right) $$

$$ FF = 1 + 4.275\ \frac{t}{c} $$

Recreated Data from DATCOM is shown in the Figure and is used to find the Appropriate Scale Factor for use in the DATCOM Equation through interpolation. $$ FF = \left[1 + L\ \left(\frac{t}{c}\right) + 100\ \left(\frac{t}{c}\right)^4\right] * R_{L.S.} $$

$$ FF = 1 + 2\ \left(\frac{t}{c}\right) + 60\ \left(\frac{t}{c}\right)^4 $$

$$ FF = 1 + Z\ \left(\frac{t}{c}\right) + 100\ \left(\frac{t}{c}\right)^4 $$ $$ Z = \frac{\left(2-M^2\right) \cos\left(\Lambda_{\frac{c}{4}}\right)} {\sqrt{1-M^2\cos^2\left(\Lambda_{\frac{c}{4}}\right)}} $$

$$ FF = 1 + \frac{2.2 \cos^2\left(\Lambda_{\frac{c}{4}}\right)} {\sqrt{1-M^2\cos^2\left(\Lambda_{\frac{c}{4}}\right)}} \left(\frac{t}{c}\right) + \frac{4.84 \cos^2\left(\Lambda_{\frac{c}{4}}\right) \left(1 + 5\cos^2\left(\Lambda_{\frac{c}{4}}\right)\right)} {2\left(1-M^2\cos^2\left(\Lambda_{\frac{c}{4}}\right)\right)} \left(\frac{t}{c}\right)^2 $$

$$ FF = 1 + 2.7\ \left(\frac{t}{c}\right) + 100\ \left(\frac{t}{c}\right)^4 $$

$$ FF = 1 + 1.8\ \left(\frac{t}{c}\right) + 50\ \left(\frac{t}{c}\right)^4 $$

$$ FF = 1 + 1.44\left(\frac{t}{c}\right) + 2\left(\frac{t}{c}\right)^2 $$

$$ FF = 1 + 1.68\left(\frac{t}{c}\right) + 3\left(\frac{t}{c}\right)^2 $$

$$ F^* = 1 + 3.3\left(\frac{t}{c}\right) - 0.008\left(\frac{t}{c}\right)^2 + 27.0\left(\frac{t}{c}\right)^3 $$ $$ FF = \left(F^* - 1\right)\left(cos^2\left(\Lambda_{\frac{c}{2}}\right)\right) + 1 $$

$$ F^* = 1 + 3.52\left(\frac{t}{c}\right) $$ $$ FF = \left(F^* - 1\right)\left(cos^2\left(\Lambda_{\frac{c}{2}}\right)\right) + 1 $$ $$ Q = 1.2 $$

Slender body form factor equations are typically given in terms of the fineness ratio (FR), which is the length to diameter ratio for the body.

$$ FR = \frac{l}{d}$$

For bodies of arbitrary cross section, an equivalent diameter is calculated based on the cross sectional area.

$$ d = 2 * \sqrt{\frac{A_{xsec}}{\pi}}$$

$$ FF = 1 + \frac{60}{FR^3} + 0.0025\ FR $$

$$ FF = 1 + \frac{0.35}{FR} $$

$$ FF = 1 + \frac{1.5}{\left(FR\right)^{1.5}} + \frac{7}{\left(FR\right)^3} $$

$$ FF = 1 + \frac{2.2}{\left(FR\right)^{1.5}} + \frac{3.8}{\left(FR\right)^3} $$

$$ FF = 1 + \frac{2.8}{\left(FR\right)^{1.5}} + \frac{3.8}{\left(FR\right)^3} $$

$$ FF = 1.02\left(1.0 + \frac{1.5}{\left(FR\right)^{1.5}} + \frac{7.0}{\left(FR\right)^3 \left(1.0 - M^3\right)^{0.6}}\right) $$

$$ \Lambda = \left(\frac{l_{r}}{\frac{4}{\pi}A_{x}}\right)^{0.5} $$ $$ FF = 1 + \frac{2.2}{\Lambda^{1.5}} - \frac{0.9}{\Lambda^3} $$

Jenkinson suggests a constant Form Factor for typical nacelles on wings. $$ FF = 1.25 $$

Jenkinson suggests a constant Form Factor for typical nacelles on aft fuselages. $$ FF = 1.50 $$

On the Overview tab, the Parasite Drag Tool includes several options for atmosphere models as well as the option for the user to have manual control over certain atmospheric qualities. The freestream type is identified by the choice labeled “Atmosphere”, and the sliders below will activate or deactivate depending on this selection. The first two freestream types are the US Standard Atmosphere 1976 and USAF 1966 atmospheric models, for which a comparison is shown below$^{16, 17}$. Note, the upper limit for the US Standard Atmospheric model is 84,852 meters, and the upper limit for the USAF model is 82,021 feet. Both require freestream velocity and altitude to be input, but an additional delta temperature input is available to offset temperature from the atmospheric model. The remaining atmosphere options require a series of manual inputs to calculate the atmospheric condition, but will not calculate and update the altitude slider. In addition, if the atmospheric choice type is “Re/L + Mach Control”, no additional properties of the flow will be calculated (i.e. pressure and density).

$ \beta \equiv \mbox{}1.458E10^{-6} \frac{kg}{(s*m*K^{1/2})} $
$ \mu \equiv \mbox{Dynamic Viscosity} $
$ S \equiv \mbox{Sutherland's Constant = 100.4 K} $

$$ \mu = \frac{\beta \cdot T^{3/2}}{T + S} $$

$ \frac{t}{c} \equiv \mbox{thickness to chord ratio of selected geometry} $
$ M \equiv \mbox{freestream Mach number for flight condition} $
$ M_{cr} \equiv \mbox{Critical Mach number, the point at which drag creep begins to occur} $
$ M_{DD} \equiv \mbox{Drag Divergence Mach number, the point at which drag significantly begins to rise} $
$ M_{DD,eff} \equiv \mbox{Effective Drag Divergence Mach number, Drag Divergence Mach number with consideration fro wing sweep} $
$ \Delta_{CD} \equiv \mbox{Additional CD due to Transonic Drag effects} $
$ \phi_{25} \equiv \mbox{Average quarter chord sweep of selected geometry} $
$ \gamma \equiv \mbox{Specific heat ratio; typically 1.4} $
$ C_{L} \equiv \mbox{Design Lift Coefficient} $

Example plots are given showing Drag Divergence Mach number using each equation with contours of quarter chord sweep angle at 0°, 15°, 30°, 45°, 60°, and 75° utilizing the following inputs: $$ C_{L} = 1.0 $$ $$ Airfoil Type = Conventional $$ $$ \gamma = 1.4 $$ $$ A_{F} = 0.8 $$ $$ K_{A} = 0.8 $$

$$ \Delta_{CD} = 20 * \left(M - M_{cr}\right)^4 $$

$ M^{*} \equiv \mbox{1.0, conventional airfoils; maximum t/c at about 0.30c} $
$ M^{*} \equiv \mbox{1.05, high-speed (peaky) airfoils, 1960-1970 technology} $
$ M^{*} \equiv \mbox{1.12 to 1.15, supercritical airfoils [Conservative = 1.12; Optimistic = 1.15]} $
$$ M_{DD,eff} = M_{DD} * \sqrt{\cos{\phi_{25}}} $$ $$ \frac{t}{c} = 0.30\cos{\phi_{25}}\left(\left(1 - \left( \frac{5 + {M_{DD,eff}}^2}{5 + {M^*}^2}\right)^{3.5}\right)\frac{\sqrt{1 - {M_{DD,eff}}^2}}{{M_{DD,eff}}^2}\right)^{\frac{2}{3}} $$

$ M^{*} \equiv \mbox{1.0, conventional airfoils; maximum t/c at about 0.30c} $
$ M^{*} \equiv \mbox{1.05, high-speed (peaky) airfoils, 1960-1970 technology} $
$ M^{*} \equiv \mbox{1.12 to 1.15, supercritical airfoils [Conservative = 1.12; Optimistic = 1.15]} $
$$ M_{DD,eff} = M_{DD} * \sqrt{\cos{\phi_{25}}} $$ $$ \frac{t}{c} = 0.30\cos{\phi_{25}}\left(\left(1 - \left( \frac{5 + {M_{DD,eff}}^2}{5 + \left(k_{M} - 0.25c_{l}\right)^2}\right)^{3.5}\right)\frac{\sqrt{1 - {M_{DD,eff}}^2}}{{M_{DD,eff}}^2}\right)^{\frac{2}{3}} $$

Equation solved for M. $$ A = \frac{M^2\cos^2{\phi_{25}}}{\sqrt{1-M^2\cos^2{\phi_{25}}}}\left(\left(\frac{\gamma + 1}{2}\right)\frac{2.64\frac{t}{c}}{\cos{\phi_{25}}} + \left(\frac{\gamma + 1}{2}\right)\frac{2.64\left(\frac{t}{c}\right)\left(0.34C_{L}\right)}{\cos^3{\phi_{25}}}\right) $$ $$ B = \frac{M^2\cos^2{\phi_{25}}}{1-M^2cos^2{\phi_{25}}}\left(\left(\frac{\gamma + 1}{2}\right)\left(\frac{1.32\frac{t}{c}}{\cos{\phi_{25}}}\right)^2\right) $$ $$ C = M^2cos^2{\phi_{25}}\left(1 + \left(\frac{\gamma + 1}{2}\right)\frac{\left(0.68C_{L}\right)}{\cos^2{\phi_{25}}} + \frac{\gamma + 1}{2}\left(\frac{0.34C_{L}}{\cos^2{\phi_{25}}}\right)^2\right) $$

$$ A + B + C - 1 = 0 $$

If a Peaky Airfoil Type is selected $$ M_{DD} = M + 0.06 $$ otherwise $$ M_{DD} = M $$

$ M_{cc} \equiv \mbox{Crest Critical Mach number} $
$$ a = 0.2 $$ $$ b = 2.131 $$ $$ x = \frac{\frac{t}{c}}{\cos{\phi_{25}}} $$ $$ y = \frac{C_{L}}{{\left(\cos{\phi_{25}}\right)}^2} $$

$$ M_{cc} = \frac{2.8355x^2 - 1.9072x + 0.949 - a\left(1-bx\right)y}{\cos{\phi_{25}}} $$

If Conventional Airfoil Type: $$ \Delta_{CD} = 0.04 $$ If Peaky Airfoil Type: $$ \Delta_{CD} = 0 $$ If Supercritical Conservative: $$ \Delta_{CD} = -0.04 $$ If Supercritical Optimistic: $$ \Delta_{CD} = -0.06 $$

$$ M_{DD} = M_{cc} * \left(1.025 + 0.08\left(1-\cos{\phi_{25}}\right)\right) - \Delta_{CD} $$

$ A_{F} \equiv \mbox{Airfoil Technology Factor, typically between 0.8 and 0.95} $
$$ M_{DD,eff} = M_{DD} * \sqrt{\cos{\phi_{25}}} $$ $$ M_{DD,eff} = A_{F} - 0.1C_{L} - \frac{t}{c} $$

$$ \frac{t}{c} = 0.7185 + 3.107e^{-5}\phi_{25} - 0.1298C_{L} - 0.7210M_{DD} $$

$ K_{A} \equiv \mbox{Airfoil Technology Factor, typically between 0.8 and 0.9} $
$$ M_{DD} = \frac{K_{A}}{cos{\phi_{25}}} - \frac{\frac{t}{c}}{cos^2{\phi_{25}}} - \frac{C_{L}}{10cos^3{\phi_{25}}} $$

$$ a = -1.147 $$ $$ b = 0.2 $$ $$ c = 0.838 $$ $$ d = 4.057 $$ $$ M_{DD} = a (C_{L} - b)d + c + \frac{30}{27}\left(\frac{t}{c} - 0.113\right) + 0.00288\left(\phi_{25} - 29.8\right) $$

$$ M_{cr} = M_{DD} $$

$$ M_{cr} = M_{DD} - 0.02 $$

$$ M_{cr} = M_{DD} - 0.1 $$

$$ M_{cr} = M_{DD} - \left(\frac{1}{80}\right)^{\frac{1}{3}} $$

1. Hoerner, S. F. (1965). Fluid-Dynamic Drag. Brick Town: Hoerner Fluid Dynamics.
2. White, F. M., Christoph, G. H. (1971). A Simple New Analysis of Compressible Turbulent Two-Dimensional Skin Friction Under Arbitrary Conditions. Dayton: Air Force Flight Dynamics Laboratory.
3. White, F. M. (2006). Viscous Fluid Flow. New York: McGraw-Hill.
4. Covert, E. E. (1985). Thrust and Drag: Its Prediction and Verification. New York: American Institute of Aeronautics and Astronautics, Inc.
5. Anderson, J. D. Jr. (1991). Fundamentals of Aerodynamics. New York: McGraw-Hill.
6. Schlichting, H. (1987). Boundary Layer Theory. New York: McGraw-Hill.
7. Gollos, W. W. (1953). Boundary Layer Drag For Non-Smooth Surfaces. Santa Monica: USAF Project RAND.
8. Jenkinson, L., Simpkin, P., & Rhodes, D. (1999). Civil Jet Aircraft Design. Reston: American Institute of Aeronautics and Astronautics.
9. Schemensky, R. T. (1973). Development of an Empirically Based Computer Proram to Predict the Aerodynamic Characteristics of Aircraft. Springfield: National Technical Information Service.
10. Feagin, R. C. (1978). Delta Method, An Empirical Drag Buildup Technique. Burbank: Lockheed.
11. McDonnell Douglas Astronautics Company. (1979). The USAF Stability and Control Digital DATCOM. St. Louis.
12. Williams, M. H. (2009, February 15). Purdue University AA251 Class Notes. Retrieved from Purdue University - College of Engineering: http://aae.www.ecn.purdue.edu/~aae251/Lectures_Fall02/class13.pdf Internet Archive
13. Kroo, I. (2009, February 15). Stanford University AA241 Class Notes. Retrieved from Stanford University: http://adg.stanford.edu/aa241/AircraftDesign.html
14. Torenbeek, E. (1982). Synthesis of Subsonic Airplane Design. Holland: Delft University Press.
15. Shevell, R. S. (1988). Fundamentals of Flight. Pearson.
16. National Aeronautics and Space Administration. (1976). U.S. Standard Atmosphere, 1976. Washington, D.C.: National Aeronautics and Space Administration.
17. United States Air Force. (1966). Flight Test Engineering Handbook. Edwards Air Force Base: United States Air Force.
18. Shevell, R. S. (2005, February 25). Development of a method for predicting the drag divergence Mach number and the drag due to compressibility for conventional and supercritical wings. Retrieved from Stanford University: http://dlib.stanford.edu:6520/text1/dd-ill/drag-divergence.pdf.
19. Howe, D. (2000). Aircraft Conceptual Design Synthesis. London: Professional Publishing.
20. Weisshaar, T.A. (2004, November 11). Weight and drag estimation : AAE 451 Aircraft Design. Retrieved from Purdue: http://roger.ecn.purdue.edu/~weisshaa/aae451/lectures.htm.
21. Böttger (1993). Entwurf einer Fluzeugfamilie als Konkurrenz zur Boeing 747-400 und Boeing 777-300. Hamburg: Deutsche Aerospace Airbus.
22. Raymer, D. P. (1992). Aircraft Design: A Conceptual Approach. Washington D.C.: AIAA Education Series.
23. Obert, E. (1997). Aircraft Design and Aircraft Operation. Linköping: Linköping Institute of Technology.
24. Roskam, J. (1989). Airplane Design. Vol. 2: Preliminary Configuration Design and Integration of the Propulsion System. Ottawa: Analysis and Research Corporation.
25. White, F. M. (2003). Fluid Mechanics, 5th Edition. New York: McGraw-Hill.