First published online July 23, 2003
Flexural stiffness in insect wings II. Spatial distribution and dynamic wing bending
S. A. Combes* and
T. L. Daniel
Department of Biology, University of Washington, Seattle, WA 98195,
USA

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Fig. 1. Unloaded (A) and loaded (B) Manduca sexta wing illuminated with
laser lines. A Matlab program was used to find the center of a laser line
running from the base of the wing to the tip before and after applying a point
force at the tip (yellow and red lines, respectively). The change in position
of the laser line y(x) was then used to find displacement of
the wing (x).
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Fig. 2. Finite element models based on Manduca sexta wings. (A) Model wing
with membrane elements (blue) and vein elements (pink), each of homogeneous
material stiffness E. (B) Model wing in which declining material
stiffness of membranes and veins results in an exponential decline in flexural
stiffness. Each color represents a different value of material stiffness.
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Fig. 3. Flexural stiffness distribution in wings of Manduca sexta and
Aeshna multicolor, and in finite element models of M. sexta
wings. In each graph, spanwise flexural stiffness is shown above (longer
lines) and chordwise flexural stiffness below; dorsal measurements are in
black and ventral measurements in gray. Each line within these groups
represents the flexural stiffness distribution estimated from wing
displacement measurements performed on a different individual. (A) Flexural
stiffness distribution of male Manduca sexta forewings (N=9
spanwise, N=10 chordwise), and of finite element models with
homogeneous (blue) and exponentially declining (red) vein and membrane
material stiffness. (B) Flexural stiffness distribution of female Manduca
sexta forewings (N=4 spanwise, N=9 chordwise). (C)
Flexural stiffness distribution of male Aeshna multicolor forewings
(N=8). (D) Flexural stiffness distribution of male Aeshna
multicolor hindwings (N=8).
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Fig. 4. Results of static bending tests on finite element model (FEM) wings. Wings
are fixed at the base, and displacement from original position (black outline)
in the z-direction is indicated by the color bar. The FEM wing with
homogeneous membrane and vein material stiffness is shown on the left and the
wing with exponentially declining material stiffness is shown on the right.
(A) Displacement due to a point force of 0.003 N (green arrow) at the wing
tip. (B) Displacement due to a normal face load of -14.43 Pa (green arrows),
the approximate pressure on a wing during steady flight.
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Fig. 5. Sequence of images from flapping finite element model wings with
homogeneous (blue) or exponentially declining (red) vein and membrane material
stiffness. Wings are moving to the right, viewed from their leading edge.
Models are shown near the end of the simulation at the same time steps,
beginning at 0.4325 s andproceeding in 0.0029 s intervals. For a movie of the
model wings in motion, see
http://faculty.washington.edu/danielt/movies.
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© The Company of Biologists Ltd 2003