First published online June 15, 2006
Journal of Experimental Biology 209, 2535-2553 (2006)
Published by The Company of Biologists 2006
doi: 10.1242/jeb.02276
Storage and recovery of elastic potential energy powers ballistic prey capture in toads
A. Kristopher Lappin*,
Jenna A. Monroy,
Jason Q. Pilarski,
Eric D. Zepnewski,
David J. Pierotti and
Kiisa C. Nishikawa*,
Department of Biological Sciences, Northern Arizona University,
Flagstaff, AZ 86011-5640, USA

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Fig. 1. (A) Force-lever setup and (B) in situ jawjoint preparation
for measurement of contractile and elastic properties of the depressor
mandibulae muscles.
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Fig. 2. Cranium and lower jaw of Bufo showing the mouth-opening muscle
(depressor mandibulae=DM) and the largest of the mouth-closing muscles
(levator mandibulae posterior longus=LM). The jaw joint is indicated by a
white circle, and the in- and out-levers are indicated by white bars.
Contraction of the depressor mandibulae (upward arrow) produces rotation of
the lower jaw about the joint (downward arrow).
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Fig. 3. Change in length of a depressor mandibulae muscle vs time during a
load-clamp experiment. When the load is reduced (t=0), the muscle
exhibits a fast phase of shortening and a slow phase of shortening with
oscillations during the transition. To define the fast to slow phase
transition (red circle), a line representing shortening during the slow phase,
and bisecting the oscillations, was extrapolated back to its initial
intersection with the length trace. Fast phase displacement is defined as the
change in length that occurs from the initial position (t=0) to this
point of intersection. This trace corresponds to Ba 1 ( F=2.82)
in Fig. 8B.
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Fig. 4. Elastic recoil model of the toad cranium. The model includes the pair of
depressor mandibulae muscles, which originate on the cranium (ground) and
insert on the retroarticular processes of the lower jaw. Each muscle (red) was
modeled as a force generator (i.e. cross bridges) and a spring (i.e. series
elastic component) arranged in series. On each side of the cranium, the
depressor mandibulae muscle is arranged in series with an extra-muscular
spring element (blue) that represents the sum of all extra-muscular structures
that are strained by contraction of the depressor mandibulae prior to movement
(i.e. cranium and retroarticular process). The effective mass
(meff) is suspended from these springs. Effective damping
(beff) of the mass-spring system is depicted in
purple.
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Fig. 5. (A) Fit between observed and predicted displacement
(xt) vs time. Displacements from two trials (high
effort and low effort) are shown for two toads. Colors represent different
individuals. For each toad (N=4), effective mass
(meff) was estimated from anatomical data. For each
feeding trial (N=71), total displacement (xt)
vs time was estimated from digital images. The time solution for the
general equation of motion (Eqn 3) was solved to find the values of the spring
constant (kt) and damping coefficient
(beff) that provided the best fit (dotted black lines) to
the observed kinematic data. (B) Maximum instantaneous in vivo power
output of the depressor mandibulae muscles and series connective tissues
during ballistic mouth opening. Colors represent different individuals.
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Fig. 6. (A) Gape profile during prey capture (black line) synchronized with EMG
activity of the depressor mandibulae (DM, red) and levator mandibulae
posterior longus (LM, blue). The ballistic phase of mouth opening is completed
during the first 20 ms and is followed by slower mouth opening as the prey
item is transported into the oral cavity. The depressor mandibulae exhibits a
large burst of activity that precedes the onset of movement by up to 250 ms,
and a smaller burst that accompanies the increase in gape angle during prey
transport. The levator mandibulae shows low-level activity before movement,
followed by a large-amplitude burst during mouth closing. Neither muscle is
active during ballistic mouth opening. (B) Examples of depressor mandibulae
activity during a trial with a smaller total displacement
(xt=2.8 mm, 0.16 ML, above) vs
a trial with a larger total displacement (xt=3.3
mm, 0.19 ML, below). Both trials are from the same toad (Ba 2).
During the trial with the larger total displacement, the depressor mandibulae
exhibits greater amplitude and a longer duration of activity prior to movement
than during the trial with the smaller total displacement. Vertical lines
delineate the ballistic phase of mouth opening. (C) Relationship between total
integrated area of depressor mandibulae activity (mVs) preceding movement and
total displacement (mm) during ballistic mouth opening (N=2). (D)
Relationship between distance to prey (cm) and duration of depressor
mandibulae activity prior to movement (N=4). Colors represent
different individuals.
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Fig. 7. (A) Lengthtension curves for the depressor mandibulae muscle
(N=3). At resting length (arrow), the muscle is at its optimum length
(L0), and a small amount of passive tension ( 0.1 N)
is present. Below resting length, active and passive tension decline rapidly.
Colors represent different individuals (lines are best least-squares fit to
third-order polynomials). Black dotted line represents mean for all
individuals combined. (B) Forcevelocity curves for the depressor
mandibulae muscle (N=3). For the three individuals,
Vmax was 3.74, 3.62, and 3.48 ML
s1. P=observed force,
P0=maximum isometric force, V=observed velocity,
Vmax=maximum shortening velocity. Colors represent
different individuals (lines are best least-squares fit to Eqn 7). Black
dotted line represents mean for all individuals combined.
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Fig. 8. Original data from 200 ms load-clamp experiments. (A) Change in length,
force and stimulation (black line) vs time for load-clamp trials at a
high clamp force (2.60 N, blue lines) and a low clamp force (0.31 N, red
lines). The depressor mandibulae muscles were stimulated isometrically for 200
ms before the load was reduced. (B) Original records of force (left) and
change in length (right) vs time from load-clamp experiments
(N=3 toads). Numbers to the right of the force traces indicate change
in load ( F). Note that length traces (right) begin 200 ms
after the onset of muscle stimulation.
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Fig. 10. Elastic properties of extra-muscular connective tissues. (A) Time course of
depressor mandibulae shortening, which equals total stretch of extra-muscular
connective tissues at the origin and insertion, measured using digital imaging
during in situ muscle stimulation. (B) Depressor mandibulae force
vs depressor mandibulae shortening. The slope is equal to the spring
constant of the extra-muscular connective tissues (ke),
which averaged 1300 N m1. (C) Relative depressor mandibulae
shortening (L/L0) as a function of relative
muscle force (P/P0). Colors represent different
individuals (N=3). Black dotted lines in B and C represent mean for
all individuals combined.
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Fig. 12. (A) Displacement (xm, xe,
xt) predicted by the elastic recoil model as a function of
the force developed by the depressor mandibulae muscles prior to movement. At
all but the lowest forces (>0.25 N), the depressor mandibulae muscles
(xm) contribute more to total displacement
(xt) than the extra-muscular connective tissues
(xe). (B) Load-dependence of the relationship between
depressor mandibulae force prior to movement (Fbefore) and
total stiffness (kt). The loads illustrated include 10
times the in vivo load (0.89 N, blue line), 5 times the in
vivo load (0.45 N, brown line), twice the in vivo load (0.18 N,
yellow line) and the observed in vivo load (0.09 N, black line), half
the in vivo load (0.045 N, green line), and one tenth the in
vivo load (0.009 N, red line). (C) Observed vs predicted
relationship between the depressor mandibulae force prior to movement
(Fbefore) and total stiffness (kt).
The solid line shows the total stiffness predicted by the elastic recoil model
at the in vivo load. Dotted lines represent the 95% confidence
interval. Colored symbols show the observed relationship between depressor
mandibulae force prior to movement (Fbefore) and total
stiffness (kt) for each individual toad (mean
± s.e.m.) estimated by fitting the observed kinematic data to
Eqn 3.
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© The Company of Biologists Ltd 2006