|
| ![]() |
|
||
| Home Help Feedback Subscriptions Archive Search Table of Contents | ||||
First published online October 19, 2007
Journal of Experimental Biology 210, 3789-3797 (2007)
Published by The Company of Biologists 2007
doi: 10.1242/jeb.006296
Modulation of pectoralis muscle function in budgerigars Melopsitaccus undulatus and zebra finches Taeniopygia guttata in response to changing flight speed

Institute of Integrative and Comparative Biology, University of Leeds, Leeds LS2 9JT, UK
Author for correspondence (e-mail:
g.n.askew{at}leeds.ac.uk)
Accepted 20 August 2007
| Summary |
|---|
|
|
|---|
Key words: flight, power, modulation, strain, recruitment, intermittent flight
| Introduction |
|---|
|
|
|---|
A number of mechanisms can vary muscle power output. First, muscles or
motor units that that have different physiological properties can be recruited
in a task-specific manner. Muscles differ widely in the stress that they can
generate, the rate at which they are able to shorten and the degree of
curvature of their force–velocity relationships
(Josephson, 1993
). All of
these factors affect the power that can be generated, resulting in a wide
range of measured skeletal muscle power outputs, from 0.5 W
kg–1 in eel slow muscle
(Ellerby et al., 2001
) to 390
W kg–1 in blue-breasted quail pectoralis muscle
(Askew and Marsh, 2001
). In
essence, power output can be increased by recruiting faster contracting
muscles or motor units (Altringham and
Johnston, 1990
; Jayne and
Lauder, 1994
; James et al.,
1995
; Wakeling,
2004
). Second, the number of motor units recruited within a given
muscle may be varied as a means of modulating muscle force output. For
example, in the lateral gastrocnemius muscle in running turkeys, motor unit
recruitment progressively increases with steeper inclines
(Roberts et al., 1997
). Third,
where an organism moves through a fluid, the muscular power source can simply
be turned off periodically to control average power output. This occurs in
fish during `burst and coast' swimming, and birds during intermittent flight.
These strategies may have an added benefit by reducing overall power
requirements relative to those associated with constant power output
(Videler and Weihs, 1982
;
Rayner, 1985
). Fourth,
fascicle strain trajectory and its relationship with muscle activity, key
determinants of muscle mechanical performance
(Marsh, 1999a
;
Askew and Marsh, 2001
), may
also be changed to control muscle power output. The strain–activity
relationship determines whether the muscle acts as (1) a power source,
primarily being active during fascicle shortening, as in the power-producing
muscles of swimmers and fliers (Altringham
and Ellerby, 1999
; Biewener et
al., 1992
); (2) an economical force producer, acting isometrically
as in the distal limb muscles of many terrestrial animals
(Roberts et al., 1997
); or (3)
is active while being stretched by an external load and absorbs mechanical
energy acting as a brake or stabiliser
(Marsh, 1999b
). In
power-producing systems, more subtle manipulations of strain trajectory can
modulate the power output of the muscle
(Askew and Marsh, 1997
;
Askew and Marsh, 1998
). Within
limits, increasing strain amplitude increases the work done by the muscle per
strain cycle (Askew and Marsh,
1998
). Changing the strain cycle frequency can change the rate at
which that work is done (Askew and Marsh,
1997
; Askew and Marsh,
1998
). Changes in the relative proportion of the strain cycle
spent shortening can also affect power output. An asymmetrical strain cycle,
in which a greater proportion of the cycle is spent shortening than
lengthening, generates a greater power output than a symmetrical cycle
(Askew and Marsh, 1997
;
Girgenrath and Marsh, 1999
).
Ultimately, however, the scope for changing strain trajectory is limited by
the intrinsic physiological properties of the muscle concerned.
The mechanical power for avian flight is primarily supplied by the
pectoralis muscles. The power output of these muscles must be modulated to
meet speed-related changes in flight power requirements. Some birds are
constrained in terms of the mechanisms they can employ to modulate pectoralis
muscle power output. Many smaller bird species, including the zebra finch and
budgerigar, have homogeneous pectoral muscles consisting of a single fibre
type, fast oxidative glycolytic (FOG)
(Rosser and George, 1986
).
This prevents them from recruiting motor units with different intrinsic
properties. Intermittent flight strategies and/or manipulations of the
relationship between muscle strain and activity are therefore the only power
modulation mechanisms that are available to them. The extent to which these
different mechanisms are used to modulate pectoralis muscle power output has
not been quantified.
The primary aim of this study was to determine the relative importance of
different power modulating mechanisms in budgerigars Melopsitaccus
undulatus and zebra finches Taeniopygia guttata across a range
of flight speeds. We measured muscle in vivo pectoralis fascicle
strain and activity during wind tunnel flight by sonomicrometry and
electromyography (EMG), respectively. Kinematic data obtained simultaneously
by high-speed video recordings were also used to examine intermittent flight
strategies. As well as indicating power modulation strategies at the muscle
level, the strain and activation data obtained are used in the companion paper
(Ellerby and Askew, 2007
) to
determine pectoralis power output in vitro using the work-loop
technique (Josephson, 1985
).
We will test the hypothesis that the speed-related changes in power
requirements can be met by modulating the activity and strain pattern of the
pectoralis muscle.
| Materials and methods |
|---|
|
|
|---|
|
Training regimens were similar for both species. We exercised the birds in the wind tunnel once a day. The amount of time spent in the wind tunnel was increased incrementally until the birds could sustain at least 15 min of continuous, steady flight at 10 m s–1 (zebra finch) or 12 m s–1 (budgerigars). This typically took 2–3 weeks. Once this level of endurance had been reached, the birds were exposed to a wide range of speeds from 4 up to 14 m s–1 (zebra finch) or 16 m s–1 (budgerigars). The speed range was dictated by the level of endurance of the birds at its extremes. At the extremes of this range the birds could not sustain steady flight for more than 30 s without becoming fatigued and landing on the bottom of the working section. A small hole in the side of the wind tunnel allowed a perch to be introduced into the front of the working section. The birds were trained to land on the perch when it was presented to them and to start flying, then land on the bottom of the working section when it was withdrawn.
Design and implantation of EMG electrodes and sonomicrometry crystals
For each experiment we constructed a set of implants consisting of two 1.0
mm sonomicrometry transducers, two bipolar EMG electrodes and a single ground
wire. These were soldered to a female, double row, eight-way PCB socket (1.27
mm pitch, zebra finch connector; 2 mm pitch, budgerigar connector). The
soldered terminals were sealed with epoxy resin. The total mass of the implant
was 0.7 g for zebra finches and 1.5 g for budgerigars.
Prior to surgery the birds were given a dose of analgesic (Vetergesic, Reckitt Benckiser Healthcare (UK) Ltd, Hull, UK; 20 µg buprenorphine hydrochloride kg–1 body mass, by intramuscular injection into the gastrocnemius muscle) and antibiotic (Baytril, Bayer Healthcare, Bury St Edmunds, UK; 10 mg enrofloxacin kg–1 body mass, by injection into the gastrocnemius muscle). Transducers and electrodes were implanted under isoflurane anaesthesia, induced at 3% concentration in oxygen and maintained at 1% concentration. Feathers were removed from small (1.5 cmx1.5 cm) areas of skin overlying the pectoralis and the dorsal surface of the pelvis. The exposed areas were swabbed with betadeine antiseptic and isolated with sterile drapes. A 1 cm skin incision was made with a scalpel at each site. A path between the two incision sites was opened by blunt dissection of the sub-cutaneous connective tissue. The transducer and EMG wires were passed along this path from the dorsal to the pectoral incision site.
To enable secure anchoring of the sonomicrometry transducers, 1.5 mm side arms were attached to the transducer wires with epoxy resin. These were made from a bent stainless steel insect pin, and oriented perpendicular to the wire 2.5 mm from the transducers. To insert a transducer into the muscle a 0.5 mm cut was made in the muscle fascia, parallel to the long axis of the fascicles, using the cutting edge of a hypodermic needle. The fascicles were separated using fine forceps, the transducer pushed into the resulting hole and the side arms sutured to the muscle fascia (using 6.0 silk suture). A second transducer was inserted in the same manner, approximately 8 mm from the first, along the same muscle fascicle.
The EMG electrodes were constructed from twisted pairs of 0.075 mm diameter Teflon coated silver wire (Goodfellow Cambridge Ltd, Cambridge, UK). The bared tips were 1 mm in length and separated by an offset of 2 mm. These were inserted into the pectoralis muscle, parallel to the muscle fascicles and adjacent to the sonomicrometry transducers, using a 25-gauge hypodermic needle with a blunted internal cutting edge, then secured by suturing to the muscle fascia (using 6.0 silk suture).
The skin incisions were closed with 5.0 silk suture. The PCB connector was left protruding from the dorsal site, anchored firmly to the skin with suture. Budgerigars were fitted with a `tunic' made from Vetrap bandage (3M, Neuss, Germany). This covered both incision sites and the connector while allowing complete freedom of movement during recovery. After cessation of anaesthesia the birds regained consciousness within 5 min. They were left to recover for between 24 and 48 h before performing the flight experiments.
The wind tunnel
The wind tunnel had a working section of 52 cmx52 cmx95 cm
(widthxheightxlength). It was constructed from transparent
PerspexTM. The back wall (viewed laterally) was spray-painted matt black
to avoid generating reflected images during filming. Vertical nylon line (0.4
mm diameter) spaced 15 mm apart upstream and 7.5 mm downstream, restricted
birds to the working section of the wind tunnel.
Camera setup and kinematic analysis
The birds were filmed using a Kodak Motion Corder high-speed camera (model
SR500; San Diego, CA, USA) at a frame rate of 125 Hz. The camera was sited
lateral and perpendicular to the working section of the wind tunnel. A mirror
was mounted at a 45° angle above the working section of the tunnel,
providing a simultaneous lateral and top view of the bird. Birds were filmed
the day before implantation of transducers and EMG electrodes, and during
collection of in vivo data post-implantation. The camera was
triggered using an external TTL input generated with a signal generator
(Wavetek, San Diego, CA, USA). This was recorded as an additional analogue
data channel input along with the in vitro data, allowing
synchronisation of these data with the video images.
The stroke amplitude, stroke plane angle relative to the horizontal, relative duration of time spent flapping, and the frequency with which non-flapping intervals occurred were quantified in the birds while uninstrumented, and post-instrumentation during collection of sonomicrometry and EMG data. The onset of non-flapping phases in finches can be easily determined as the wings are fully withdrawn and held against the body. In budgerigars, intermittent flight behaviour is more complex as the wings are held partly outstretched between bouts of flapping. Despite this, the distinction between the flapping phases, with high amplitude wing tip movements, and the non-flapping phases with little or no wing tip movement and partial wing retraction, is clear.
Experimental protocols
Instrumented birds were placed in the wind tunnel while wrapped in a soft
cloth to prevent them from reaching the wires and connectors. After connection
of the dorsal connector to the data cable the bird was released and allowed to
sit on the perch at the front of the working section. The wind tunnel was set
to 10 m s–1 and the bird flown for a short time to allow
adjustment of sonomicrometer triggering levels. Data were subsequently
collected at 2 ms–1 intervals over a range of speeds, from 4
to 16 m s–1 in budgerigars, and at 0 and from 4 to 14 m
s–1 in zebra finches. Flight was initiated by withdrawing the
perch. At each speed we waited until the bird was flying steadily, then
initiated saving of the in vivo data and triggered the camera. At 125
Hz frame rate the camera could store 18 s of video images in its internal
memory. Once the data were saved the perch was reintroduced and the bird was
allowed to rest for approximately 2 min while the video segment was saved onto
digital video tape. After completion of data collection the birds were
euthanized by cervical dislocation. The placement of the transducers and EMG
electrodes in the pectoralis muscle was confirmed by dissection.
Signal processing and data collection
The implants in the bird were linked to the external equipment via
a lightweight data cable. This was 1.5 m long and consisted of a twisted pair
of insulated 42-gauge copper wires linked to each sonomicrometer transducer, a
pair of 0.07 mm enamelled copper wires linked to each EMG electrode, and a
single 0.07 mm enamelled copper wire acting as a ground wire. These were
soldered to a male PCB connector that was attached to the connector on the
bird. The total mass of the cable and proximal connector was 0.65 and 1.37 g
for zebra finch and budgerigars, respectively. The individual wires were kept
bundled together with cyanoacrylate adhesive applied at intervals along its
length. The cable exited the working section via a small dorsal hole
and connected to a junction box placed on top of the wind tunnel. This was
linked to pre-amplifiers and the sonomicrometer via shielded cables.
The junction box and all the peripheral equipment were linked to a common
ground. EMG signals were recorded via pre-amplifiers (DAM50, WPI,
USA) at a gain of 1000 and a 10 kHz low-pass filter applied. The two EMG
channels were collected as additional analogue inputs using the A to D boards
of the sonomicrometer system (TRX Series 8, Sonometrics, Ontario, Canada) at a
sampling rate of 2.1 kHz. All data were stored on the hard drive of a PC.
Data handling and analysis
The in vivo data were exported as text files using Sonometrics
SonoLAB software (Version 3.4.25, Sonometrics, Ontario, Canada). All
subsequent data handling and analysis was carried out using Igor Pro (Version
5.0.1.0, WaveMetrics, USA). A digital high-pass filter, designed with the Igor
IFDL filter design package, was applied to the EMG data to remove movement
artefacts. Sonomicrometry data are subject to two main types of error: those
caused by high-frequency electrical noise riding on the transducer signals,
and level shifts caused by changes in transducer signal strength. We were
fortunate that the environment in which we carried out the experiments was
largely free of electrical noise. Level shifts, as the name suggests, are
apparent instantaneous changes in length. These are a consequence of the way
in which the sonomicrometer measures length by triggering of the `ringing'
signal created by a high-frequency voltage pulse applied to the piezoelectric
transducer. A series of voltage peaks is generated by the oscillation of the
transducer. Ideally, length is measured by triggering off the first peak.
Changes in signal strength occasionally result in a shift in triggering to a
subsequent voltage peak. These artefacts were removed using an Igor macro
(designed by R. L. Marsh) that moved the portion of trace after the level
shift back down to the pre-shift level.
Only segments of steady flying in the centre of the working section were selected for analysis. For each individual and speed, 16 wingbeats were analysed to extract basic EMG and strain parameters. We determined EMG onset and offset times for these wingbeats. Filtered EMG waves were rectified and the integral over the EMG burst calculated. This was divided by burst duration to determine EMG intensity. To enable comparison between individuals, EMG intensity was scaled relative to the mean intensity at the highest flight speed, where the maximum intensity was typically recorded. We also determined the time and muscle segment length at the maximum and minimum of each strain cycle. These data were used to calculate strain amplitude, strain cycle frequency, and the relative durations of muscle lengthening and shortening within each cycle.
All statistical analyses were carried out using SPSS (Version 11.0, SPSS Inc., USA). A general linear model (GLM) was used to test for changes in EMG and strain parameters with flight speed. A GLM was also used to test for changes in flight performance as a result of surgical implantation by comparing pre- and post-surgical flight kinematics. In all models speed was treated as an independent variable, and an identifier of each individual bird included as a random factor. For muscle function analyses, the dependent variables were relative EMG intensity, EMG timing relative to peak muscle length, EMG duty cycle (EMG duration expressed as a proportion of strain cycle duration), strain cycle frequency, strain amplitude, and the proportion of the strain cycle spent shortening. For kinematic analyses, the dependent variables were wingbeat frequency, amplitude and stroke plane angle, and the proportion of flight time spent flapping the wings. All proportional data were arcsine-transformed prior to analysis. Where significant speed effects were detected by the GLM, Scheffé's post-hoc test was used to perform pairwise comparisons between mean values. This test was selected as it is relatively conservative in terms of declaring measured differences as being statistically significant.
| Results |
|---|
|
|
|---|
|
|
|
|
Muscle strain modulation with flight speed
A significant change in the overall pectoral muscle strain with flight
speed was detected in both zebra finches (GLM, F=8.26,
P<0.001, Fig. 3C)
and budgerigars (GLM, F=4.85, P=0.002,
Fig. 4C). Strain was lowest at
intermediate speeds in both species. In both species the range of strain
measured across the range of speeds studied was similar: 0.12–0.15 in
budgerigar and 0.13–0.16 in zebra finch. We also detected significant
changes in strain cycle frequency (and concomitant changes in wingbeat
frequency) with flight speed in both species (GLM, F=8.14,
P<0.001, zebra finches, Fig.
3D; GLM, F=3.35, P=0.014, budgerigar,
Fig. 4D). Wingbeat frequency in
both species was highest (16 Hz in budgerigar and 30 Hz in zebra finch) at the
highest flight speed and had a minimum at an intermediate speed. The degree of
asymmetry of the strain cycle in terms of the relative amounts of time spent
lengthening and shortening was also quantified. We detected no significant
changes in relative shortening duration in in zebra finches (GLM,
F=1.71, P=0.154, Fig.
3E), but did detect a significant change in budgerigars (GLM,
F=3.26, P=0.016, Fig.
4E). In zebra finches the overall mean relative shortening
duration was 0.67±0.10 (mean ± 1 s.d.), whereas in budgerigars
the range was 0.56–0.69.
Flight kinematics
Kinematic data were collected from both species before implantation of
sonomicrometry transducers and EMG electrodes, and subsequently in the same
individuals after implantation during collection of pectoralis muscle fascicle
strain and activity data. We detected no effect of instrumenting the birds on
stroke amplitude in zebra finches (GLM, F=0.211, P=0.665,
Fig. 5A), but detected a
significant change in budgerigars (GLM, F=7.36, P=0.03,
Fig. 6A). Stroke amplitude
changed significantly with speed in zebra finches (GLM, F=27.8,
P<0.001, Fig. 5A),
but not in budgerigars (GLM, F=0.80, P=0.578,
Fig. 6A). No effect of
instrumentation on stroke plane angle was detected in either species (GLM,
F=0.02, P=0.901, zebra finches,
Fig. 5B; GLM, F=0.61,
P=0.462, budgerigars, Fig.
6B). Stroke plane angle changed significantly with speed in both
species (GLM, F=14.10, P<0.001, zebra finches,
Fig. 5B; F=57.97,
P<0.001, budgerigars, Fig.
6B).
|
|
Because all the individual zebra finches bounded with the wings held
against the body, at all speeds, wing kinematics during the non-flapping phase
was not quantified in this species. Budgerigars typically held their wings
partially outstretched in the non-flapping phase. As there was potential for
speed- or instrumentation-related changes in this behaviour we quantified the
relative wingspan (non-flapping span, relative to maximum wingspan) during
this phase. We detected no significant changes due to instrumentation (GLM,
F=0.02, P=0.886), or speed changes (GLM, F=1.18,
P=0.323) in the relative wingspan of the budgerigars during the
non-flapping phase (Fig. 6E).
The absence of speed-related changes is in contrast to previous work with this
species that showed a progressive retraction of the wings during the
non-flapping phase with increasing speed
(Tobalske and Dial, 1994
).
| Discussion |
|---|
|
|
|---|
In terms of speed-related changes in EMG intensity, budgerigars show a
greater scope (1.60-fold) than zebra finches (1.34-fold overall, 1.27-fold,
forward flight). The detailed neuromuscular organization of the pectoralis
muscles in these species is unknown. As the pectoralis muscles in both species
consist of a single muscle fibre type
(Rosser and George, 1986
), EMG
intensity changes likely indicate changes in the level of motor unit
recruitment in the muscle across the speed range, rather than the progressive
recruitment of increasingly fast fibre types seen in the mixed fibre type
muscle systems of most other vertebrates. If all other factors that determine
muscle power and force production remained unchanged, then this would indicate
simple modulation of muscle force, with consequent changes in muscle work
output per wingbeat. Changes in fascicle strain trajectory in concert with
those in EMG intensity prevent a straightforward link between EMG intensity
and muscle force being established for the pectoralis muscles of either
species.
Both budgerigars and zebra finches modulated fascicle strain. In budgerigars, the observed scope for changing strain amplitude was 1.32, relative to 1.23 in zebra finches. Beyond this, the strain modulation patterns of the two species diverge. The shape of the strain cycle, in terms of relative time spent shortening, did not change significantly with speed in zebra finch (Fig. 3E), whereas the scope for change was greater in budgerigars (scope 1.24, Fig. 4E). The only parameter in which zebra finches showed greater scope for change than budgerigars was strain cycle frequency, where the scope was 1.16, relative to 1.07 in budgerigars.
In both species, the observed changes in recruitment and fascicle strain
trajectory are consistent with meeting flight power requirements that change
in a U-shaped pattern with speed (Askew and
Ellerby, 2007
; Rayner,
1999
; Ellerby and Askew,
2007
). EMG intensities, synonymous with increased force
production, are highest at the extremes of the speed ranges
(Fig. 3B,
Fig. 4B). Muscles have distinct
optima for the strain and frequency at which power output is maximal, as shown
by in vitro physiological studies
(Stokes and Josephson, 1988
;
Josephson and Stokes, 1989
;
Askew and Marsh, 1997
) and
mathematical models (Weis-Fogh and
Alexander, 1977
; Josephson and
Stokes, 1989
; Josephson,
1989
). The proportion of the strain cycle spent shortening has
also been shown to be an important determinant of muscle power output, with
power increasing as the proportion of the cycle spent shortening increases
(Askew and Marsh, 1997
). Where
differences in strain amplitude, strain cycle frequency and asymmetry were
detected, the conditions most likely to maximise power output occurred at the
upper and lower extremes of the speed range (Figs
3,
4). In some muscles the
relationship between strain trajectory and activation recorded in
vivo during activities that demand high mechanical powers (such as sound
production or escape locomotion) have been shown in vitro to
correspond to those that are optimal for maximising power output
(Askew and Marsh, 2001
;
Girgenrath and Marsh, 1999
).
In flying vertebrates, it seems reasonable to hypothesise that at the upper
and lower extremes of the speed range, where flight power requirements are
highest, the flight muscles operate under conditions that are optimal for
maximising power output. At intermediate speeds, the reduced power
requirements can be met by the flight muscles operating under sub-optimal
conditions. Our measurements on the pectoralis muscle in budgerigars and zebra
finches support this hypothesis, in that where these parameters are modulated,
strain cycle amplitude, asymmetry and frequency are reduced at intermediate
flight speeds (Figs 3,
4).
In budgerigars, the minima for EMG intensity, strain, and relative
shortening duration all occurred at 8–10 m s–1
(Fig. 4B,C,E), suggesting that
this may be the minimum power speed. This corresponds closely to the speed at
which metabolic power, as measured by respirometry, is lowest in this species
(Tucker, 1968
;
Bundle et al., 2007
). No
metabolic power-speed data are available for zebra finches; however our in
vivo muscle strain and activity data suggest a minimum power speed lying
between 4 and 8 m s–1
(Fig. 3). For both species, the
strain and activity parameters that show variation show minima at flight
speeds that closely correspond to the speed at which mechanical power is
lowest, as measured in vitro and as estimated from an aerodynamic
analysis (Askew and Ellerby,
2007
; Ellerby and Askew,
2007
).
The largely U-shaped relationships between relative EMG intensity and
flight speed observed in budgerigars and zebra finches in the present study,
and a previous study on zebra finches
(Tobalske et al., 2005
), are
absent in some other studies. In European starlings Sturnus vulgaris,
relative EMG intensity increased 1.4-fold with increasing speed between 8 and
16 m s–1 (Tobalske,
1995
). In budgerigars, relative EMG intensity increased 1.4-fold
with increasing speed between 7 and 13 m s–1
(Tobalske and Dial, 1994
). The
different patterns may be due to the narrower range of flight speeds used in
these previous studies. It is likely that 8 m s–1 in
starlings is close to the minimum power speed
(Ward et al., 2001
) and 7 m
s–1 in budgerigars is only a little below the minimum power
speed (Ellerby and Askew,
2007
). Therefore it might be expected that relative EMG intensity
and wingbeat frequency will increase at speeds below the minima investigated.
The only comparable muscle strain and activity data in the literature that
cover a broad range of flight speeds are from the cockatiel [Nymphicus
hollandicus (Hedrick et al.,
2003
)], where the scope for changing strain cycle amplitude,
relative shortening duration and frequency was 1.29, 1.24 and 1.24,
respectively. EMG intensity also was also correlated with measured muscle
force in this species, indicating power modulation through changes in motor
unit recruitment in addition to changes in strain trajectory.
Where data are available, it is clear that birds are manipulating strain trajectory and motor unit recruitment to modulate pectoralis power output across a range of flight speed. There is, however, a high degree of interspecific variation in terms of the scope for change in the various parameters that can be changed to modulate power output at the muscle level. Even the budgerigar and cockatiel, which are both in the family Psittacidae, show different patterns of strain trajectory change. The extent to which both species can change strain amplitude (scope 1.29 cockatiel, 1.32 budgerigar) and relative shortening duration (scope 1.24 cockatiel, 1.24 budgerigar) are very similar, but wingbeat frequency changes much more in cockatiels (scope 1.24) than in budgerigars (scope 1.07). Given the limited data available for comparison, any patterns relating to phylogeny or scaling are currently impossible to discern.
While our data are indicative of power modulation with speed at the muscle
level, it is difficult to draw conclusions about the relative importance of
changes in recruitment and strain trajectory without making direct
measurements of muscle mechanical performance. Unless all other factors that
influence power output remain equal, changes in one parameter cannot
meaningfully be related to likely changes in muscle power output. The primary
determinants of muscle power output are the intrinsic physiological properties
of the muscle, the time-course of muscle activation, the level of motor unit
recruitment and the strain trajectory of the muscle
(Josephson, 1999
). The
shortening or lengthening velocity of the muscle is determined by the length
trajectory and is therefore affected by the shape of the length trajectory,
the cycle frequency and strain. A simple change in the level of motor unit
recruitment, indicated by changes in EMG intensity would be indicative of
changes in muscle force production. However, where this occurs in concert with
any change in the muscle's length trajectory, this link can no longer be
established. Changes in the length trajectory alter where the muscle operates
on the length–force relationship (strain and mean muscle length) and
force–velocity curve (strain, frequency, and shape), and change the
relative importance of mechanisms such as stretch activation and shortening
deactivation (Askew and Marsh,
1998
; Josephson,
1999
). This means that attempting to discern the relative
importance of different power modulation mechanisms by component analysis
(e.g. Hedrick et al., 2003
) is
ultimately fruitless because of the complex inter-relationship between the
various factors affecting muscle force production.
|
Fixed gear models of this type are underpinned by the basic force–velocity relationship of muscles in vitro. Under conditions of isovelocity shortening the power output of most muscles is maximised at a shortening velocity of approximately one-third of the maximal shortening velocity (Vmax). Therefore, to preserve optimum muscle function in terms of maximising power output, it is argued that fascicle shortening velocity should be maintained within narrow limits across a range of flight speeds. This does not necessarily imply that the overall strain trajectory should remain constant, but that the cumulative effects of changing cycle frequency, amplitude, and shape should preserve the shortening velocity of the fascicles when active.
A more detailed examination of the physiological properties of muscle
leaves this line of reasoning open to question for a number of reasons. (1)
Even under conditions of simple, isovelocity shortening, the velocity range at
which power output is close to maximal is actually quite broad. In the mouse
soleus muscle the optimal shortening velocity to maximise power output is
0.22Vmax, but 90% of maximum power output is achieved over
a range of velocities from approximately 0.15 to 0.35Vmax
(Askew and Marsh, 1998
). (2)
Data obtained from isovelocity measurements are difficult to relate to
complex, cyclically operating systems. This is particularly true where
shortening velocity is not constant, as in the avian pectoralis muscle
(Askew and Marsh, 2001
) (see
Figs 1,
2). (3) In vitro
force–velocity measurements are typically made in fully activated
muscle. In the avian pectoralis, the fascicles are stretched while being
activated, and shorten while deactivating (Figs
1,
2). Changes in the rate of
stretch and shortening will also affect stretch activation and shortening
deactivation (Askew and Marsh,
1998
). For example, increasing the velocity of shortening during
relaxation facilitates deactivation. (4) Where the proportion of the cycle
spent shortening changes, as in the budgerigar, optimal
V/Vmax also changes
(Askew and Marsh, 1998
). So,
while muscles are clearly constrained by their intrinsic contractile
properties, we should expect those constraints to be broader than suggested by
standard force–velocity relationships. This is borne out by the fact
that the average shortening velocity showed considerable plasticity across the
speed range in both species (Fig.
7), changing significantly with speed (F=3.31,
P=0.015, budgerigars; F=3.81, P=0.006, zebra
finches), the scope for changing shortening velocity being 1.23 and 1.36 in
budgerigars and zebra finches, respectively. Thus the argument that
intermittent flight may allow average muscle power output to be modulated
while preserving an optimal V/Vmax is over
simplistic. This does not rule out intermittent flight behaviour as a power
modulation mechanism. Both budgerigars and zebra finches tended to spend
proportionally less time flapping their wings at intermediate speeds where
power requirements are lowest (Fig.
5C, Fig. 6C). This
is consistent with the use of intermittent flight as a simple power modulation
strategy by periodically turning off the mechanical power source to control
the average power output over time. Overall, however, the idea that
intermittent flight serves to maintain a `fixed gear' fails to recognise the
plasticity in function at the muscle level, and intermittent flight should be
seen as being only one component of a complex power modulation strategy in
both species.
| Acknowledgments |
|---|
| Footnotes |
|---|
| References |
|---|
|
|
|---|
Alexander, R. M. (2005). Mechanics of animal movement. Curr. Biol. 15,R616 -R619.[CrossRef][Medline]
Altringham, J. D. and Johnston, I. A. (1990).
Modelling muscle power output in a swimming fish. J. Exp.
Biol. 148,395
-402.
Altringham, J. D. and Ellerby, D. J. (1999). Fish swimming: patterns in muscle function. J. Exp. Biol. 202,3397 -3403.[Abstract]
Askew, G. N. and Ellerby, D. J. (2007). The
mechanical power requirements of avian flight. Biol.
Lett. 3,445
-448.
Askew, G. N. and Marsh, R. L. (1997). The effects of length trajectory on the mechanical power output of mouse skeletal muscles. J. Exp. Biol. 200,3119 -3131.[Abstract]
Askew, G. N. and Marsh, R. L. (1998). Optimal shortening velocity (V/Vmax) of skeletal muscle during cyclical contractions: length–force effects and velocity-dependent activation and deactivation. J. Exp. Biol. 201,1527 -1540.[Abstract]
Askew, G. N. and Marsh, R. L. (2001). The
mechanical power output of the pectoralis muscle of blue-breasted quail
(Coturnix chinensis): the in vivo length cycle and its
implications for muscle performance. J. Exp. Biol.
204,3587
-3600.
Biewener, A. A., Dial, K. P. and Goslow, G. E.
(1992). Pectoralis muscle force and power output during flight in
the starling. J. Exp. Biol.
164, 1-18.
Bundle, M. W., Hansen, K. S. and Dial, K. P.
(2007). Does the metabolic rate–flight speed relationship
vary among geometrically similar birds of different mass? J. Exp.
Biol. 210,1075
-1083.
Cavagna, G. A., Heglund, N. C. and Taylor, C. R. (1977). Mechanical work in terrestrial locomotion II. Basic mechanisms for minimizing energy expenditure. Am. J. Physiol. 233,R243 -R261.[Medline]
Ellerby, D. J. and Askew, G. N. (2007).
Modulation of flight muscle power output in budgerigars Melopsittacus
undulatus and zebra finches Taeniopygia guttata: in
vitro muscle performance. J. Exp. Biol.
210,3780
-3788.
Ellerby, D. J. and Marsh, R. L. (2006). The
energetic costs of trunk and distal-limb loading during walking and running in
guinea fowl Numida meleagris: II. Muscle energy use as indicated by
blood flow. J. Exp. Biol.
209,2064
-2075.
Ellerby, D. J., Spierts, I. L. Y. and Altringham, J. D. (2001). Slow muscle power output of yellow- and silver-phase European eels (Anguilla anguilla L.): changes in muscle performance prior to migration. J. Exp. Biol. 204,1369 -1379.[Abstract]
Gabaldon, A. M., Nelson, F. E. and Roberts, T. J.
(2004). Mechanical function of two ankle extensors in wild
turkeys: shifts from energy production to energy absorption during incline
versus decline running. J. Exp. Biol.
207,2277
-2288.
Girgenrath, M. and Marsh, R. L. (1999). Power output of sound-producing muscles in the tree frogs Hyla versicolor and Hyla chrysoscelis. J. Exp. Biol. 202,3225 -3237.[Abstract]
Hedrick, T. L., Tobalske, B. W. and Blewener, A. A.
(2003). How cockatiels (Nymphicus hollandicus) modulate
pectoralis power output across flight speeds. J. Exp.
Biol. 206,1363
-1378.
James, R. S., Altringham, J. D. and Goldspink, D. F. (1995). The mechanical properties of slow and fast skeletal muscles of the mouse in relation to their locomotory function. J. Exp. Biol. 198,491 -502.[Medline]
Jayne, B. C. and Lauder, G. V. (1994). How swimming fish use slow and fast muscle fibers – implications for models of vertebrate muscle recruitment. J. Comp. Physiol. A 175,123 -131.[Medline]
Josephson, R. K. (1985). Mechanical power
output from striated-muscle during cyclic contraction. J. Exp.
Biol. 114,493
-512.
Josephson, R. K. (1989). Power output from
skeletal muscle during linear and sinusoidal shortening. J. Exp.
Biol. 147,533
-537.
Josephson, R. K. (1993). Contraction dynamics and power output of skeletal muscle. Annu. Rev. Physiol. 55,527 -546.[CrossRef][Medline]
Josephson, R. K. (1999). Dissecting muscle power output. J. Exp. Biol. 202,3369 -3375.[Abstract]
Josephson, R. K. and Stokes, D. R. (1989).
Strain, muscle length and work output in a crab muscle. J. Exp.
Biol. 145,45
-61.
Marsh, R. L. (1999a). Contractile properties of muscles used in sound production and locomotion in two species of gray tree frog. J. Exp. Biol. 202,3215 -3223.[Abstract]
Marsh, R. L. (1999b). How muscles deal with real-world loads: the influence of length trajectory on muscle performance. J. Exp. Biol. 202,3377 -3385.[Abstract]
Rayner, J. M. V. (1985). Bounding and undulating flight in birds. J. Theor. Biol. 117, 47-77.[CrossRef]
Rayner, J. M. V. (1999). Estimating power curves of flying vertebrates. J. Exp. Biol. 202,3449 -3461.[Abstract]
Roberts, T. J. and Scales, J. A. (2002).
Mechanical power output during running accelerations in wild turkeys.
J. Exp. Biol. 205,1485
-1494.
Roberts, T. J., Marsh, R. L., Weyand, P. G. and Taylor, C.
R. (1997). Muscular force in running turkeys: the economy of
minimizing work. Science
275,1113
-1115.
Rosser, B. W. C. and George, J. C. (1986). The avian pectoralis: histochemical characterization and distribution of muscle fiber types. Can. J. Zool. 64,1174 -1185.[CrossRef]
Stokes, D. R. and Josephson, R. K. (1988). The
mechanical power output of a crab respiratory muscle. J. Exp.
Biol. 140,287
-299.
Tobalske, B. W. (1995). Neuromuscular control and kinematics of intermittent flight in the European starling (Sturnus vulgaris). J. Exp. Biol. 198,1259 -1273.[Medline]
Tobalske, B. W. and Dial, K. P. (1994). Neuromuscular control and kinematics of intermittent flight in budgerigars (Melopsittacus undulatus). J. Exp. Biol. 187, 1-18.[Abstract]
Tobalske, B. W., Puccinelli, L. A. and Sheridan, D. C.
(2005). Contractile activity of the pectoralis in the zebra finch
according to mode and velocity of flap-bounding flight. J. Exp.
Biol. 208,2895
-2901.
Tucker, V. A. (1968). Respiratory exchange and
evaporative water loss in flying budgerigar. J. Exp.
Biol. 48,67
-87.
Videler, J. J. and Weihs, D. (1982). Energetic
advantages of burst and coast swimming of fish at high speeds. J.
Exp. Biol. 97,169
-178.
Wakeling, J. M. (2004). Motor units are
recruited in a task-dependent fashion during locomotion. J. Exp.
Biol. 207,3883
-3890.
Ward, S., Moller, U., Rayner, J. M. V., Jackson, D. M., Bilo,
D., Nachtigall, W. and Speakman, J. R. (2001). Metabolic
power, mechanical power and efficiency during wind tunnel flight by the
European starling Sturnus vulgaris. J. Exp. Biol.
204,3311
-3322.
Weis-Fogh, T. and Alexander, R. McN. (1977). The sustained power output from skeletal muscle. In Scale Effects in Animal Locomotion (ed. T. J. Pedley), pp.511 -525. London: Academic Press.
![]()
CiteULike
Complore
Connotea
Del.icio.us
Digg
Reddit
Technorati
Twitter What's this?
This article has been cited by other articles:
![]() |
D. J. Ellerby and G. N. Askew Modulation of flight muscle power output in budgerigars Melopsittacus undulatus and zebra finches Taeniopygia guttata: in vitro muscle performance J. Exp. Biol., November 1, 2007; 210(21): 3780 - 3788. [Abstract] [Full Text] [PDF] |
||||
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||