Weakfish sonic muscle: influence of size, temperature and season
M. A. Connaughton1,*,
M. L. Fine2 and
M. H. Taylor3
1 Washington College, Department of Biology, 300 Washington Avenue,
Chestertown, MD 21620, USA
2 Department of Biology, Virginia Commonwealth University, Richmond, VA
23284-2012, USA
3 College of Marine Studies and Department of Biological Sciences,
University of Delaware, Newark, DE 19716, USA

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Fig. 2. Sonogram (A) and oscillogram (B) of a typical weakfish disturbance call
consisting of a series of individual pulses of sound. Expanded oscillogram (C)
of a single pulse consisting of 2-3 cycles of acoustic energy. Spectrum (D) of
the pulse in C, demonstrating a dominant frequency of 480 Hz. Figures taken
from Connaughton et al.
(1997 ).
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Fig. 3. Relationship between dominant frequency and pulse duration for (A) fish
ranging from 25 to 36 cm in total length (recorded at 18 °C,
N=11) and (B) fish recorded at 12, 18 and 23 °C (28-31 cm in
total length, N=8). (C) A plot of dominant frequency divided by a
frequency calculated from the period of the second cycle of acoustic energy
(shaded bar in inset). Frequency was calculated as [1000/(the duration of the
second cycle of acoustic energy)]. Note that the dominant frequency is closely
matched (expressed as values near to 1) by the inverse of the duration of the
second cycle of acoustic energy. Figures modified from Connaughton et al.
(2000 ).
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Fig. 4. Frequency and time-domain responses of low- and high-Q resonators. Acoustic
data from a single weakfish pulse (A,B) express a wide bandwidth (arrows in A)
and short duration (B, total duration less than 5 ms), typical of a low-Q,
broadly tuned resonator. Acoustic data from a 440Hz tuning fork (C,D) express
a narrow bandwidth (arrows in C) and a long duration (D, total duration more
than 10s), common to a high-Q, tuned resonator (after
Bradbury and Vehrenkamp, 1998 ).
The time scales in C and D are the same as those in A and B.
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© The Company of Biologists Ltd 2002