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Birds

Storyboard

Birds have a very unique way of flying that sets them apart from the techniques used by humans in their aircraft. In this case, the wings serve a dual purpose, generating both lift and thrust, even when the bird is stationary.

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ID:(2056, 0)



Mechanisms

Iframe

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Code
Concept
Example of wing factors
Pigeon flight study, front view
Pigeon flight study, side view
Wing shape

Mechanisms

Example of wing factorsPigeon flight study, front viewPigeon flight study, side viewWing shape

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Pigeon flight study, side view

Concept

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If you study the video of a pigeon flying from a lateral perspective, you can observe how it advances and retracts its wings.

None

During the forward phase, the bird manages to generate lift, while during the backward phase, it seeks propulsion.

ID:(1587, 0)



Pigeon flight study, front view

Concept

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If you study the video of a pigeon flying from a frontal perspective, you can observe how it extends and retracts its wings.

None

During the forward phase, the bird extends its wings for the first time to generate lift, while during the backward phase, it extends them for the second time to propel itself forward.

ID:(1589, 0)



Wing shape

Description

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To model the wing, we need to estimate the wing span (L), the width the wing width (w), and the wing height (d) of the wing in order to calculate the surface that generates lift (S_w) and the total object profile (S_p). An article with data for migratory birds can be found in [1]:

Bird m [kg] S_w [m2] L [m] \Delta [m]
Stonechat 0.0232 0.01366 0.264 0.052
Meadow Pipit 0.0199 0.0143 0.273 0.052
Nightingale 0.0197 0.01059 0.221 0.048
Barn Swallow 0.0182 0.01446 0.328 0.044
Robin 0.0182 0.01026 0.224 0.046
Yellow Wagtail 0.0176 0.01051 0.248 0.042
Spotted Flycatcher 0.0153 0.01209 0.262 0.046
Black Redstart 0.015 0.01006 0.200 0.050
Garden Warbler 0.0123 0.00779 0.200 0.039
Pied Flycatcher 0.012 0.00873 0.200 0.044
Serin 0.0114 0.00828 0.214 0.039
Garden Warbler 0.0087 0.00768 0.194 0.040
Goldcrest 0.0054 0.00504 0.146 0.035

Note: In this case, wing areas and spans are provided, so the width can be estimated as S_w/L. Similarly, the wing height can be estimated from the profile area divided by the span S_p/L, although in this case, we are not considering that the profile includes the bird's body section.

[1] "Field Estimates of Body Drag Coefficient on the basis of dives in passerine Birds," Anders Hedenström, Felix Liechti, The Journal of Experimental Biology, 204, 1167-1175 (2001).

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Example of wing factors

Image

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When we compare different types of wings, we notice that raptors tend to have shorter and broader wings, whereas migratory birds have longer and narrower ones. Therefore, it makes sense to define the aspect Ratio (\gamma_w) as the relationship between the wing span (L) and the wing width (w):

None

ID:(7043, 0)



Model

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Parameters

Symbol
Text
Variable
Value
Units
Calculate
MKS Value
MKS Units
\gamma_w
gamma_w
Aspect Ratio
-
S_w
S_w
Surface that generates lift
m^2
\gamma_d
gamma_d
Thickness to span ratio
-
S_p
S_p
Total object profile
m^2
d
d
Wing height
m
L
L
Wing span
m
w
w
Wing width
m

Variables

Symbol
Text
Variable
Value
Units
Calculate
MKS Value
MKS Units

Calculations


First, select the equation: to , then, select the variable: to
gamma_r = d / w gamma_w = w / L P_w = rho * L ^2* C_w * v ^3/(2* gamma_p )+2* m ^2* g ^2* gamma_w /( c ^2* L ^2* rho * v ) S_p = L * d S_w = L * D gamma_wS_wgamma_dS_pdLw

Calculations

Symbol
Equation
Solved
Translated

Calculations

Symbol
Equation
Solved
Translated

Variable Given Calculate Target : Equation To be used
gamma_r = d / w gamma_w = w / L P_w = rho * L ^2* C_w * v ^3/(2* gamma_p )+2* m ^2* g ^2* gamma_w /( c ^2* L ^2* rho * v ) S_p = L * d S_w = L * D gamma_wS_wgamma_dS_pdLw




Equations

#
Equation

\gamma_r =\displaystyle\frac{ d }{ w }

gamma_r = d / w


\gamma_w =\displaystyle\frac{ w }{ L }

gamma_w = w / L


P_w =\displaystyle\frac{1}{2} \rho L ^2 C_w v ^3\displaystyle\frac{1}{ \gamma_p }+\displaystyle\frac{2 m ^2 g ^2}{ c ^2 L ^2 \rho } \gamma_w \displaystyle\frac{1}{ v }

P_w = rho * L ^2* C_w * v ^3/(2* gamma_p )+2* m ^2* g ^2* gamma_w /( c ^2* L ^2* rho * v )


S_p = L \delta

S_p = L * d


S_w = L \Delta

S_w = L * D

ID:(15191, 0)



Wing surface

Equation

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The surface that generates lift (S_w) can be estimated using the wing span (L) and the wing width (w) as follows:

S_w = L \Delta

S_w
Surface that generates lift
m^2
6117
L
Wing span
m
6337
\Delta
Wing width
m
6336
gamma_w = w / L S_w = L * D S_p = L * d gamma_r = d / w P_w = rho * L ^2* C_w * v ^3/(2* gamma_p )+2* m ^2* g ^2* gamma_w /( c ^2* L ^2* rho * v )gamma_wS_wgamma_dS_pdLw

ID:(4553, 0)



Wing profile perpendicular to the direction of flight

Equation

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The total object profile (S_p) can be estimated using the wing span (L) and the wing height (d) as follows:

S_p = L \delta

S_p
Total object profile
m^2
6123
\delta
Wing height
m
6338
L
Wing span
m
6337
gamma_w = w / L S_w = L * D S_p = L * d gamma_r = d / w P_w = rho * L ^2* C_w * v ^3/(2* gamma_p )+2* m ^2* g ^2* gamma_w /( c ^2* L ^2* rho * v )gamma_wS_wgamma_dS_pdLw

ID:(4554, 0)



Aspect Ratio

Equation

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The aspect Ratio (\gamma_w) is defined as the ratio between the wing width (w) and the wing span (L), indicating the proportion or relationship between these two variables:

\gamma_w =\displaystyle\frac{ w }{ L }

\gamma_w
Aspect Ratio
-
6334
L
Wing span
m
6337
w
Wing width
m
6336
gamma_w = w / L S_w = L * D S_p = L * d gamma_r = d / w P_w = rho * L ^2* C_w * v ^3/(2* gamma_p )+2* m ^2* g ^2* gamma_w /( c ^2* L ^2* rho * v )gamma_wS_wgamma_dS_pdLw

ID:(4551, 0)



Thickness ratio

Equation

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The aspect Ratio (\gamma_w) can be defined as the thickness to span ratio (\gamma_d), which relates the wing width (w) to ($$)6338

\gamma_r =\displaystyle\frac{ d }{ w }

\gamma_r
Thickness to span ratio
-
6344
d
Wing height
m
6338
w
Wing width
m
6336
gamma_w = w / L S_w = L * D S_p = L * d gamma_r = d / w P_w = rho * L ^2* C_w * v ^3/(2* gamma_p )+2* m ^2* g ^2* gamma_w /( c ^2* L ^2* rho * v )gamma_wS_wgamma_dS_pdLw

ID:(4555, 0)



Power as a function of wing and profile factors

Equation

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Just as the power of flight (P) is related to the density (\rho), the total object profile (S_p), the coefficient of resistance (C_W), the body mass (m), the gravitational Acceleration (g), the proportionality constant coefficient sustainability (c), the surface that generates lift (S_w), and the speed with respect to the medium (v) through

P =\displaystyle\frac{1}{2} \rho S_p C_W v ^3 + \displaystyle\frac{2 m ^2 g ^2}{ c ^2 S_w \rho }\displaystyle\frac{1}{ v }

,

we can express the power in terms of the aspect Ratio (\gamma_w) and the thickness to span ratio (\gamma_d) as

P_w =\displaystyle\frac{1}{2} \rho L ^2 C_w v ^3\displaystyle\frac{1}{ \gamma_p }+\displaystyle\frac{2 m ^2 g ^2}{ c ^2 L ^2 \rho } \gamma_w \displaystyle\frac{1}{ v }

gamma_w = w / L S_w = L * D S_p = L * d gamma_r = d / w P_w = rho * L ^2* C_w * v ^3/(2* gamma_p )+2* m ^2* g ^2* gamma_w /( c ^2* L ^2* rho * v )gamma_wS_wgamma_dS_pdLw

As the power of flight (P) is related to the density (\rho), the total object profile (S_p), the coefficient of resistance (C_W), the body mass (m), the gravitational Acceleration (g), the proportionality constant coefficient sustainability (c), the surface that generates lift (S_w), and the speed with respect to the medium (v) through

P =\displaystyle\frac{1}{2} \rho S_p C_W v ^3 + \displaystyle\frac{2 m ^2 g ^2}{ c ^2 S_w \rho }\displaystyle\frac{1}{ v }

,

with the definitions of the surface that generates lift (S_w) in terms of the wing width (w)

S_w = L \Delta

,

and the aspect Ratio (\gamma_w)

\gamma_w =\displaystyle\frac{ w }{ L }

,

along with the aircraft body mass (m_p) in relation to the wing height (d)

S_p = L \delta

,

and the thickness to span ratio (\gamma_d)

\gamma_r =\displaystyle\frac{ d }{ w }

,

finally, as

P_w =\displaystyle\frac{1}{2} \rho L ^2 C_w v ^3\displaystyle\frac{1}{ \gamma_p }+\displaystyle\frac{2 m ^2 g ^2}{ c ^2 L ^2 \rho } \gamma_w \displaystyle\frac{1}{ v }

.

.

ID:(9593, 0)