First published online January 27, 2004
Journal of Experimental Biology 207, 767-776 (2004)
Published by The Company of Biologists 2004
doi: 10.1242/jeb.00817
A hierarchical analysis of the scaling of force and power production by dragonfly flight motors
Rudolf J. Schilder* and
James H. Marden
208 Mueller Laboratory, Department of Biology, Pennsylvania State
University, University Park, PA 16802, USA

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Fig. 1. Schematic representation of a basalar muscle and its third order lever
system. FWf indicates the position of the wing fulcrum, FW represents forewing
length and Ba indicates the position of the apodeme of the basalar muscle. The
basalar muscle (yellow) produces force Fdyn, which is then
transmitted through d1, the distance between the basalar
apodeme and wing fulcrum, and d2, the second moment of
wing area where the mean aerodynamic force acts.
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Fig. 2. Example of raw data obtained during a workloop experiment. The sinusoidal
length cycles are shown in red, the timing of stimulation is shown in blue,
and resulting tension developed by the basalar muscle is shown in green.
Tension data from the fourth cycle were used for further analyses.
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Fig. 3. Detailed ventral view of the internal surface of the Anax junius
dorsal thorax at the base of the forewing, showing the location of the basalar
muscle apodeme (Ba) and the wing fulcrum (Wf) of the forewing (FW). The
distance between these two structures is the muscle apodeme-to-wing fulcrum
lever arm length (d1). All muscle tissue has been removed.
Scale bar, 1 mm. A portion of the wing is drawn to orient the reader; this
wing is not to scale.
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Fig. 4. (A) Maximum lifting force (Flift) as a function of
thorax mass (mthor).
log10Flift=1.682+1.035log10mthor
(r2=0.99; S.E.slope=0.036;
N=10). (B) Maximum isometric force (Fstat) as a
function of basalar muscle mass (mbas).
log10Fstat=2.863+0.670log10mbas
(r2=0.96; S.E.slope=0.050;
N=10). The datapoint marked `Teneral' indicates a newly
emerged and therefore physiologically immature T. lacerata. This
point was excluded from the regression analysis.
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Fig. 5. (A) Effective lever arm length (d2) as a function of
basalar muscle mass (mbas).
log10d2=0.143+0.307log10mbas
(r2=0.72; S.E.slope=0.027;
N=51). Symbols are as in B. (B) Internal lever arm length
(d1) as a function of mbas.
log10d1=0.710+0.540log10mbas
(r2=0.77; S.E.slope=0.042;
N=52).
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Fig. 6. Examples of workloops for each species. Basalar muscle length (l),
mass (m) and contraction frequency (f) are given for each
specimen.
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Fig. 7. (A) Mean dynamic force output (Fdyn) as a function of
basalar muscle mass (mbas).
log10Fdyn=3.020+0.834log10mbas
(r2=0.76; S.E.slope=0.086;
N=33). (B) Force output during one maximal-effort muscle contraction
cycle at the output end of the lever system (Find) as a
function of mbas. log10
Find=2.304+1.036log10mbas
(r2=0.83; S.E.slope=0.086;
N=33). Symbols are as in Fig.
5B.
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Fig. 8. Maximum force output as a function of motor mass for `Group 2 motors' and
single muscles (Marden and Allen,
2002 ). The upper and lower (grey) linear regression equations are
log10Max. force output=2.95+0.667log10Muscle mass and
log10Max. force output= 1.74+0.999log10Motor mass,
respectively. Blue graphs a, b, c and d represent data and scaling equations
obtained in this study. `Motor mass' is synonymous to thorax mass
(mthor) for Flift data. Basalar muscle
mass (mbas) is used for Fstat,
Fdyn and Find data.
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Fig. 9. (A) Mass-specific power (Pm) as a function of basalar
mass (mbas).
log10Pm=3.147+0.237log10mbas
(r2=0.18; S.E.slope=0.09;
N=33). (B) Mass-specific work (Wm) as a function
of mbas.
log10Wm=2.530+0.433log10mbas
(r2=0.39; S.E.slope=0.10;
N=33). Symbols are as in Fig.
5B.
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© The Company of Biologists Ltd 2004