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First published online October 5, 2006
Journal of Experimental Biology 209, 4174-4184 (2006)
Published by The Company of Biologists 2006
doi: 10.1242/jeb.02489
Escape responses in juvenile Atlantic cod Gadus morhua L.: the effects of turbidity and predator speed
1 Department of Biology, University of Bergen, PO Box 7800, Bergen N-5020,
Norway
2 CNR-IAMC, Loc. Sa Mardini, 09072 Torregrande, Oristano, Italy
3 International Marine Centre, Loc. Sa Mardini, 09072 Torregrande, Oristano,
Italy
* Author for correspondence (e-mail: Justin.Meager{at}bio.uib.no)
Accepted 10 August 2006
| Summary |
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Turbidity affected both PES and the type of escape response used by the fish, but these effects depended on predator speed. PES for the fast predator attack declined from 73% in clear water to 21% in highly turbid water, due to decreased responsiveness and poorly timed escapes. Intermediate turbidity enhanced PES and responsiveness to the slow predator attack. Locomotor performance was reduced by turbidity, whereas predator speed had the opposite effect. Our results suggest that both predator attack speed and turbidity have important roles in determining the vulnerability of fish attacked by piscivorous predators.
Key words: turbidity, predator, speed, escape response, cod, Gadus morhua
| Introduction |
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In aquatic systems, escape responses rely on sensory and motor systems that
can be affected by environmental factors such as turbidity, temperature and
dissolved oxygen (Webb and Zhang,
1994
; Miner and Stein,
1996
; Lefrancois et al.,
2005
). Vision has been studied extensively as one of the main
sensory systems involved in escape responses
(Dill, 1974a
;
Fuiman, 1993
;
Domenici, 2002
) and provides a
high spatial and temporal resolution of information of the identity, distance,
speed and direction of approaching predators
(Curio, 1993
;
Hemmi, 2005b
). Turbidity from
suspended sediment, dissolved organic matter and plankton scatters and absorbs
light and can reduce the visual abilities of fish (e.g.
Gregory and Northcote, 1993
)
(for a review, see Utne-Palm,
2002
). Turbidity may therefore shift the advantage of piscivorous
predatorprey interactions in either direction, depending on relative
effects on the detection abilities of predators and prey. Numerous studies
have looked at the effect of turbidity on detection of prey by predators (e.g.
Gregory and Northcote, 1993
;
Vogel and Beauchamp, 1999
),
but very few studies have looked at the effect of turbidity on detection of
predators by prey (Miner and Stein,
1996
).
Visual escape responses require both perception of the predator and a
decision to escape (Blaxter and Fuiman,
1990
; Hemmi,
2005a
), based on the level of perceived risk
(Ydenberg and Dill, 1986
).
Escaping from predators that pose no risk is energetically costly
(Harper and Blake, 1988
) and
occurs at the expense of other fitness related behaviours (for a review, see
Lima, 1998
). Risk of directly
approaching predators is conveyed by the magnifying retinal image; fish
usually escape when the rate of change of this signal reaches a certain
threshold (Dill, 1974a
).
Responding too early may allow predators to compensate for early reactions
(Blaxter and Fuiman, 1990
),
while escaping at the latest possible moment may be advantageous [the `matador
strategy' (Blaxter and Fuiman,
1990
; Fuiman,
1993
)].
|
As both predator speed and turbidity influence the distance from which prey
respond to predators (prey reactive distance)
(Dill, 1974a
;
Miner and Stein, 1996
), their
combined effects are likely to be more complex. While prey reactive distance
is longer for faster predators (Dill,
1974a
), it is limited by turbidity
(Miner and Stein, 1996
). We
therefore predict that turbidity will have greater effects on fast predators
(longer reactive distances) than slow predators (shorter reactive distances)
(Fig. 1).
|
This paper examines escape responses of juvenile Atlantic cod under laboratory conditions. We tested the hypothesis that the influence of turbidity on escape responses depends on predator attack speed, with greater effects at faster speeds (Fig. 1). We also aimed to determine which characteristics of an escape response are affected by turbidity and predator speed.
| Materials and methods |
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Experiments were conducted in a large rectangular glass aquarium (70
cmx300 cmx50 cm), filled to a depth of 20 cm with seawater
(salinity: 3235
, temperature: 9±1°C) from a
flow-through seawater system (Fig.
2). This depth was used so fish could be viewed from above in the
highest turbidity treatments. Prey were located in a experimental arena (5 mm
thick glass) that was lowered down into the aquarium and further separated
from the predator model by a clear, removable divide that consisted of one 5
mm thick glass sheet and one 5 mm thick Perspex sheet with rubber shock
absorbers placed between (Fig.
2). The walls of the fish compartment rested on a silicon cushion
(10 mm thick). The opposing end of the aquarium was painted white.
Diffuse light conditions were provided (9.5±0.5 µmol
m2 s1) by indirectly illuminating (lights
directed towards the white walls and ceiling of the room) the aquarium with
four halogen floodlights (2x 150 W, 2x 500 W). This irradiance
level is equivalent to that found in juvenile cod habitat in coastal waters of
western Norway [i.e. at a 20-m depth on a clear summer day or 3 m depth on a
cloudy winter day
(Bali
o and
Aksnes, 1993
)]. The experimental aquarium was illuminated from
underneath with disperse infrared light (>800 nm wavelength) and fish
silhouettes were recorded at 250 frames s1 using an overhead
high-speed video camera (Redlake Motion Scope 1000S PCI, Tucson, AZ, USA)
fitted with an infrared filter (Optolite 50% IR, Instrument Plastics Ltd.,
Maidenhead, Berks, UK). Turbidity levels were established by combining clay
particles (pulverised kaolinite, Polsperse 10, IMERYS, Oslo, Norway) and
seawater in a mixing tank and recirculating the water through the experimental
tank (Fig. 2) (for details, see
Meager et al., 2005
).
Predator model
Predator attacks were simulated by a predator model that was computer
controlled, and hence able to move through the experimental aquarium at highly
repeatable speeds. This model was based on the frontal profile of a 60 cm
generalised teleost predator, i.e. with a conical shape and 15 cm wide (i.e.
0.25 body lengths; BL) at a point 18 cm from the tip of the snout
(0.3 BL) (Domenici,
2002
). Predator length was based on field data for predators of
Atlantic cod (Scharf et al.,
2000
). The model was painted matte black to give it an inherent
contrast of 1 against the white background.
The predator model was driven by an electric motor with a variable-speed transformer. A computer server (Omron Corporation, Xmonwin 1.0) regulated model speed every 2.5 ms to maintain the predator model to within 10% of the designated speed for approximately 90% of the predator path (slow speed: 92% of path; fast speed: 87% of path). Cruising speed of the model was measured with a high-speed camera at 250 frames s1 (Redlake, Motion Scope PCI) and was the same for five separate trials of each speed. The model was then synchronised with the high-speed camera to allow us to determine the position of the predator model in each frame, at each predator speed. The predator model and high-speed camera were triggered simultaneously from a control room (5 m away).
Experimental protocol
We examined the visual-escape response of juvenile cod to two predator
model speeds: 150 cm s1 and 296 cm s1 (2.5
BL s1 and 4.9 BL s1 for
a 60 cm predator) and four turbidity levels: 0.5, 3, 6 and 14 beam attenuation
m1 (1.8, 11, 20 and 44 NTU nephelometric turbidity units,
measured using a Vernier Turbidity Sensor, Sarasota, FL, USA). Predator speeds
were based on values from a review
(Domenici, 2002
) and
turbidities represented the range of habitats used by juvenile Atlantic cod
(see Meager et al., 2005
).
Turbidity was measured as the percent of light transmitted through a 10 cm
cuvette in a spectrophotometer (Shimadzu UV-VIS Recording Spectrophotometer
UV-160, Duisburg, Germany) at 800 nm (to minimise near-forward scattering) and
converted to beam attenuation using the standard relationship:
T=expcr, where T is light transmitted
through a path length r (in m) and c is the beam attenuation
coefficient.
A minimum of 10 fish (mean total length ± 1 s.e.m.=12.9±0.1
cm; 101 fish tested in total) were tested for each predator
speedturbidity treatment. Higher numbers of fish were tested where
necessary to provide a minimum of 7 responders in each treatment. Each trial
used a different fish to avoid learning effects
(Dill, 1974b
).
After turbidity levels (±0.5 m1) were established
in the aquarium, the fish compartment and divides were lowered into place
(Fig. 2). Fish were then
transported from holding tanks using plastic bags filled with water to
minimise handling stress and each fish was acclimated to the fish compartment
for 1.5 h (Artigas et al.,
2005
). The predator stimulus and high-speed camera were triggered
when cod entered into a `target area' that was trapezium shaped (base: 15 cm,
height: 10 cm, area: 300 cm2) and 828 cm from where the
predator model stopped. We used this target area to standardise the prey's
visual perspective of the model (i.e. to avoid a lateral view of the model)
and to avoid effects of compartment walls on escape trajectories
(Eaton and Emberley, 1991
).
Prey reactions were recorded at 250 frames s1.
After each trial was completed, fish were anaesthetised and eye size (diameter; mm), standard length (cm) and weight (g) were measured. Water samples from random locations at 78 cm depth in both the predator and prey sections of the aquarium at the start and finish of each trial were used to measure turbidity during a trial.
Trials were also conducted with a black screen (0.16 mm thick black polyethylene plastic) fixed to the front of the fish compartment (Fig. 2B) to control for potential non-visual responses, e.g. due to noise or vibrations generated by the motor or predator model. 26 different fish were tested in clear (beam attenuation coefficient c=0.5 m1) and highly turbid water (c=14 m1) at both predator model speeds. No non-visual responses were recorded.
Behavioural and kinematic analysis
Trials were analysed using frame-by-frame replay (Win Analyse, Version 1.6,
Mikromak, Berlin, Germany) to measure the effect of turbidity and predator
speed on responsiveness, and escape timing, direction and locomotor
performance. The following conventions were used to analyse escape responses:
stage 1, the initial turn; stage 2, rotation of the head in the opposite
direction (Domenici and Blake,
1997
).
Responsiveness
Responsiveness (% of individuals responding to predator stimulus) was
measured for all fish tested. Fish that turned as the predator model
approached, or up to 100 ms after the model stopped, were classified as
`responders', and all other fish were classified as `non-responders'.
Escape locomotor performance
Escape locomotor performance was measured by turning rate, and distance
covered over a fixed-time interval. Turning rate was calculated as the stage 1
angle, i.e. difference in orientation of the head between the initial position
and at the end of stage 1, divided by the duration of the turn
(Domenici and Batty, 1997
).
This was determined for the midline of the fish, which was measured as the
straight line passing from the centre of mass (when stretched straight, i.e.
0.35 BL) to the tip of the head
(Domenici and Blake,
1997
).
Turning rates were used to classify escape types
(Domenici and Batty, 1997
;
Domenici et al., 2004
). To
compare escape types with turns during spontaneous swimming, we also measured
turning rates of fish of the same size range in the tank during routine
activity (i.e. same experimental conditions, but without the predator
model).
Distance covered (D80) was defined as the distance between the centre of mass of the fish at time 0 and 80 ms after the initiation of the escape response (80 ms was chosen as the maximum duration for which all escapes were in the field of view of the camera and within the propulsive phases of the escape).
Escape direction
Escape trajectory and initial orientation were determined for each fish by
measuring the angle between the midline of the fish (anterior to the centre of
mass) and the attack path of the predator (for details, see
Domenici and Blake, 1993
).
Hence, an angle of 0° represented a fish heading towards the predator.
Escape trajectory was determined as the final angle of the escape (i.e. when
the fish was swimming in a straight direction or gliding), relative to the
attack path of the predator. All fish were observed to swim on a straight
course or glide at the end of the escape response, while they were within the
field of view of the camera. Initial orientation was measured at frame 0 (1
frame before the first detectable movement).
Escape timing
Reactive distance (RD) was calculated as the distance between the
nearest prey eye and the posterior section (i.e. widest point) of the predator
model, at frame 1 (frame with first detectable movement). We also estimated
`true reactive distance' (TRD), which took into account the delay
between perception of the stimulus and the first detectable movement of fish
(or latency) (Batty and Domenici,
2000
). TRD was calculated for a range of latencies from
the literature [50 and 100 ms: based on visual escape latencies
(Batty, 1989
)].
We also calculated apparent predator size as the angular size of the
predator's image on the retina of the prey
(O'Brien et al., 1976
) (in
degrees). Apparent looming threshold (ALT) was calculated as the rate of
change of this angle (rad s1), using the following equation
(Dill, 1974a
):
![]() | (1) |
Putative escape performance (PES)
Fish were grouped into two categories: `caught' or `escaped', based on the
likelihood of escaping the initial `predator attack'. This calculation was
defined as `putative escape performance' (PES) and was based on the predator
model continuing to move in a straight line with a constant speed. We used a
predator gape size of 0.1 BL, which was representative of a
generalist predator (for a review, see
Domenici, 2002
) and within the
range of predators of juvenile Atlantic cod
(Scharf et al., 2000
). We
measured PES by superimposing the putative path of the predator model over the
prey footage. Prey were assumed to have escaped the predator once the whole
body reached the outer limit of the path of the predator's gape
projection.
Data analysis
Data were analysed using SPSS [Release 13,
(SPSS Inc., 1999-2004
)],
Statistica (Release 6.1, StatSoft Inc.,
2003
) and Oriana (Release 2.02, Kovach Computing Services). The
relationships between responsiveness, and turbidity and predator speed were
analysed using logistic regression. We also used logistic regression to test
for the influence of turbidity and speed on locomotor performance category,
and on PES. The goodness of fit of a particular model was determined using the
Likelihood Ratio statistic (G2). Logit models were used to
compare treatments and the odds of an occurrence were calculated as the
exponential transformation of the corresponding logit value
(Agresti, 1990
).
Differences in escape direction between turbidities and predator speeds
were tested using the MardiaWatsonWheeler tests
(Batschelet, 1981
).
Non-linear regression of treatment medians was used to test for the
standard relationship between turbidity (c) and reactive distance
(Gregory and Northcote, 1992). Conceptually, non-responders may have had a
higher ALT had the stimulus been close enough. Hence, ALT data were treated as
Type 1 censored samples (Webb,
1982
; Blaxter and Fuiman,
1990
) and the Generalised Wilcoxon Test
(StatSoft Inc., 2003
) test for
comparing survival curves was used to test for differences in ALT between
turbidity levels. ALT values were log-normally distributed and were
log-transformed. We also used the Generalised Wilcoxon Test to test for
differences in reactive distance between predator speeds.
To determine which factors had the most influence on PES we used
forward-stepwise logistic regression. The following variables were included:
timing (ALT and RD), locomotor performance (D80,
S1 angle, S1 duration, turning rate) and direction (escape trajectory). We
also included initial orientation in the model. In this analysis, escape
trajectory and initial orientation were transformed into angular displacement
from the predator path (i.e. from 0 to 180°)
(Batschelet, 1981
).
|
| Results |
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Escape locomotor performance
Kinematic type of escape responses
Fish evaded the model with three types of responses based on a frequency
distribution of turning rates (Fig.
4): slow responses, with turns of similar turning rates as during
routine swimming (mean turning rate ± s.e.m.) of 395.3±41.2 deg.
s1 (range: 119.6591.9 deg. s1),
intermediate responses with a mean turning rate of 1117.3±41.3 deg.
s1 (range: 942.81335.9 deg. s1) and
fast responses with a mean turning rate of 2215.7±41.2 deg.
s1 (range: 1718.53002.7 deg. s1).
These response categories differed significantly in escape speed
(D80 and S1 duration), but not in S1 angle
(Table 1; ANOVA analysis). The
average speed (over first 80 ms) of slow escape responses was 10.7±1.5
cm s1 (0.8±0.1 BL s1),
compared with 33.2±6.8 cm s1 (2.4±0.5
BL s1) for intermediate responses and
72.4±3.6 cm s1 (5.7±0.3 BL
s1) for fast responses.
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Effects of turbidity and predator speed on locomotor performance
Because of limited numbers of slow responses
(Fig. 4), slow and intermediate
responses were pooled as `slow-intermediate responses'. The proportion of
slow-intermediate responses and fast responses was significantly affected by
predator attack speed and turbidity (predator speed: G2=
10.5, d.f.=1, P=0.001; turbidity: G2=5.4, d.f.=1,
P=0.02). Slow-intermediate responses were more commonly elicited by
the slow predator attack speed and fast responses were more often triggered by
the fast predator attack. The logit model predicted that the odds of fish
responding with a fast response were 4.4 times higher for the fast predator
speed than for the slow predator speed. The proportion of slow-intermediate
responses was greater in turbid (314 m1) than clear
water (Fig. 5). The logit model
predicted that the odds of a fast response ranged from 4.2 in clear water to 1
in highly turbid water (i.e. the probability of fish responding with a fast
response in clear water was 0.81, compared with 0.5 at a turbidity of 14
m1). Although there was a trend for the proportion of fast
responses to decrease at a turbidity of 3 m1 for the slow
predator speed, and increase for the fast predator velocity, there was no
significant interaction between turbidity and predator speed (interaction
term: G2=0.01, d.f.=1, P=0.93).
|
Escape direction
Turbidity did not significantly affect the direction of escape from the
predator model (MardiaWatsonWheeler Test: W=4.79,
P=0.571, N=1721). Similarly, escape direction was not
significantly affected by predator speed (MardiaWatsonWheeler
Test: W=1.29, P=0.524, N1=31,
N2 =38). Although most fish were close to perpendicular to
the line of predator at the start of the `predator attack' (circular mean
± s.e.m. = 88.1±3.4°), initial orientations ranged from
5° to 160°. The mean escape trajectory (± s.e.m.) was
165.8±3.7° (relative to an approaching predator at 0°). The
distribution of escape trajectories, however, tended to be bimodal with peaks
around 140° and 180° (Fig.
6). There were no significant differences in direction or initial
orientation between the kinematic type of escapes
(MardiaWatsonWheeler Test: P=0.490.98).
|
Escape timing
Fish were between 206 and 225 cm from the predator model when the model was
triggered, and the model stopped between 11 and 28 cm from the initial
position of the fish (mean ± 1 s.e.m.: 18.1±5.1 cm). In clear
water, reactive distance did not significantly differ between predator attack
speeds (mean RD ± 1 s.e.m.: slow attack, 91.3±25.3 cm;
fast attack: 96.9±22.1 cm) (Generalised Wilcoxon test:
Z=0.092, P=0.089).
Reactive distance (cm) to the fast predator model declined as a negative power function of turbidity (c, m1) (RD=67.01xturbidity0.705, r2=0.99, P=0.009 for 4 treatment medians, Fig. 7A). However, the relationship between reactive distance and turbidity was not significant for the slowest predator speed (RD=70.3xturbidity0.252, r2=0.34, P=0.416 for 4 treatment medians, Fig. 7B). Apparent predator size followed an inverse function of reactive distance i.e. the predator appeared larger when it was closer (Fig. 7A,B).
|
2=14.1, d.f.=3, P=0.003; slow predator:
2=0.31, d.f.=3, P=0.96). ALT increased from clear
water (1.11±0.15 rad s1) to the highest turbidity
(2.16±1.75 rad s1) for the fast predator attack
speed, indicating a higher response threshold at higher turbidities. Mean
response threshold (ALT ± s.e.m.) was 1.11±0.15 rad
s1 to the slow predator speed (TLT50ms
=0.66±0.091 rad s1; TLT100ms
=0.55±0.081 rad s1) and 2.16±1.75 rad
s1 (TLT50ms=1.44±0.22 rad
s1, TLT100ms= 1.18±0.21 rad
s1) to the fast predator speed.
Putative escape success
None of the non-responders were likely to have evaded the simulated
predator attack. Putative escape success (PES) was significantly affected by
an interaction between turbidity and speed (interaction term:
G2=10.2, d.f.=1, P=0.001; speed:
G2=4.3, d.f.=1, P=0.38; turbidity:
G2=3.7, d.f.=1, P=0.06). PES was higher for the
slow predator speed in all turbidities except clear water
(Fig. 8A). Increasing turbidity
reduced putative escape success for the fast predator attack speed, in a
similar manner to reactive distance (Fig.
8A and Fig. 7A).
Hence, the logit model predicted that fish were 7.3 times more likely to evade
the fast predator model in clear water than in turbid water (614
m1). However, for the slowest predator speed, putative
escape success was the highest at intermediate turbidity (80% PES at
c=3 m1), but similar between clear water and other
turbidity categories (0.5, 6 and 14 m1)
(Fig. 8A).
|
We analysed `responders' separately to remove variation associated with responsiveness. An interaction between turbidity and predator attack speed also significantly influenced PES of responders (interaction term: G2=4.16, d.f.=1, P=0.041; predator speed: G2=3.68, d.f.=1, P=0.06; turbidity: G2=0.68, d.f.=1, P=0.41). Patterns of significance of PES between treatments were similar to the complete data set, i.e. PES was significantly lower in turbid water than clear water for the fast predator speed and significantly higher at 3 m1 than other turbidity levels for the slow predator speed (Fig. 8B). In contrast to the complete data set, however, PES to the fast predator speed was similar between turbidities from 3 to 14 m1 and PES was similar between predator attack speeds in clear water (logit analysis, Fig. 8A,B). 6089% of the responders escaped the slow predator model, compared with 4373% for the fast predator model (Fig. 8B).
Influence of escape parameters on putative escape success
Of the various escape parameters examined, response timing (ALT and RD) had
the greatest influence on putative escape success
(Table 2). ALT had the most
significant affect on PES, but responsiveness and reactive distance were also
significant (Table 2). Although
ALT was derived from reactive distance, ALT took into account predator speed
and predator size (Eqn 1).
|
ALT was also the most important variable affecting the fish that responded (Table 2). We also tested for other factors that may have influenced PES (minor variations in temperature, fish condition factor, eye size and length), but found no significant effects (P values from 0.108 to 0.999).
| Discussion |
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The effect of turbidity on responsiveness and response timing was more complex for the slow predator attack. Responsiveness was similar between clear water and high turbidity (614 m1), but there was an unexpected increase at intermediate turbidity (c=3 m1, Fig. 3). Reactive distance was also variable and did not follow the relationship shown for the fast predator speed (Fig. 7). Furthermore, responsiveness to the slow predator attack in clear water was considerably less than to the fast attack (Fig. 3).
It is unlikely that the fish in our experiment were less vigilant in clear
water, as all fish responded to the fast predator attack in clear water
(Fig. 3). An alternative
explanation for these results is that perceived risk to the slow predator
attack was low in clear water and increased in intermediate turbidity. In our
system, risk is represented by time to contact with the `predator' after it
enters the visual field of the prey. Hence, higher turbidity levels (and
faster predator speeds) imply increased risk. Even at intermediate turbidity,
fish have considerably less time to visually assess the risk imposed by an
approaching object and less visual information. Due to the exponential
attenuation of image-forming light in turbid water, visual distance in
intermediate turbidity is considerably less than in clear water
(Aksnes and Giske, 1993
).
Hence, the predator model was substantially closer (and appeared larger) by
the time it was first detected by prey in intermediate turbidity, compared to
clear water (Fig. 7). This
would give the predator model a tendency to rapidly increase the area of the
prey's retina stimulated in intermediate turbidity. Such a sudden appearance
of large image may have enhanced responsiveness in intermediate turbidity
(compared to clear water) by increasing perceived risk or startling the fish.
In this context, such increased perceived risk or larger retinal stimulation
may not have occurred in higher turbidity levels, because of a further
reduction of visual range at high turbidity levels (614
m1), reducing the probability of fish seeing the slow
predator model in time to respond. Contrast degradation at high turbidity
levels water may have also reduced the visual information to a level that was
below the threshold required for a response by some fish
(Aksnes and Giske, 1993
).
This explanation, however, remains speculative as we did not quantify
perceived risk (Abrahams and Dill,
1989
). Very little is known of visual predator recognition and
predator-risk assessment in conditions of poor visibility and this subject
needs further investigation. It is also interesting to note that contrary to
theoretical predictions and previous work
(Dill, 1974a
)
(Fig. 1), reactive distances
were quite similar between predator speeds in clear water. Fish therefore had
a higher response threshold (i.e. higher ALT) to the fast predator attack. The
basis for discrepancies between our results and those of Dill
(Dill, 1974a
), who obtained a
constant ALT independent of predator speed, are unclear but may be due to
differences in methodology, temporal resolution or the species used. This
indicates that further research into the relationship between predator speed
and ALT may be warranted.
Escape locomotor performance
Turbidity and predator attack speed affected escape locomotor performance.
Fish responded to the predator model with three categories of responses that
varied in turning rates, and escapes with high turning rates were more
commonly elicited by a fast predator attack and/or in clear water
(Fig. 5). Enhanced locomotor
performance to a fast predator attack speed indicates that escape responses
depended on the immediacy of the threat, i.e. faster predators need to be
evaded more quickly than slower predators. Decreased locomotor performance at
higher turbidity levels, however, seems counterintuitive as the predator model
was also closer to fish at the time of the response
(Fig. 7). This is likely to be
because of less visual information from the predator model (i.e. reduced
contrast) over a shorter duration of time, hence, fish may not have received
sufficient `threat' information.
Our results indicated that escape behaviour was not maximised as an `all or
nothing' manoeuvre and are supported by numerous other studies (e.g.
Webb, 1982
;
Webb, 1986
;
Domenici and Batty, 1994
;
Domenici and Batty, 1997
;
Domenici et al., 2004
). The
several kinematically discrete escape behaviours may be the result of
different neural circuits or muscle activation patterns, as suggested
elsewhere (Domenici and Batty,
1994
; Domenici and Batty,
1997
) [for a review of the neural basis of behaviour, see also
DiDomenico and Eaton (DiDomenico and
Eaton, 1988
)].
Neither predator speed nor turbidity affected the direction of escape
responses. Our study was the first to examine escape direction in cod and
shows that escape trajectories are similar to those found in other fish
species startled by mechano-acoustic stimuli (e.g.
Domenici and Blake, 1993
;
Domenici and Batty, 1997
). It
has been suggested that bimodal distributions of escape trajectories may imply
sensory and biomechanical optimisations
(Domenici and Blake, 1993
).
Our results suggest that escape trajectories may be relatively independent of
the sensory systems involved.
Putative escape success
Turbidity and predator attack speed affected PES in a similar way to
responsiveness. PES was largely determinant upon fish responding to the
predator attack, and responding early enough to escape (i.e. timing and
responsiveness). For example, of the 79% of fish that were `caught' by the
fast predator attack in high turbidity (14 m1,
Fig. 8A), 57% were
non-responders and the remaining 22% responded either too late or were too
slow to escape.
Fish had approximately half the time to respond to the fast predator model than to the slow predator speed (since RD was relatively constant), hence, had lower PES to the fast predator model (between turbidity levels of 3 and 14 m1, Fig. 8A). Similarly, fish had less time to evade the model as turbidity increased and visual range decreased (Fig. 7). The effects of turbidity and speed were therefore addictive, and PES was the lowest for the fast predator speed in turbid water, because fish were unable to see the model until it was close. Low PES to the slow predator attack in clear water was the exception to this pattern and was likely to be due to factors other than time/distance constraints, because the fish had considerable time to respond to the model (approx. 1.3 s) (Figs 3 and 8).
Response timing and responsiveness also determine escape success of larval
fish from a fish predator (Fuiman,
1993
) and of fish to avian predators
(Katzir, 1993
), and are
critical in determining the outcome of predatorprey interactions
(Domenici and Blake, 1997
).
Although it did not influence escape success significantly in our study,
escape locomotor performance also varied with turbidity and predator speed.
Locomotor performance is likely to be much more important in real
predatorprey interactions, where the predator pursues the prey after
the first strike (Webb, 1986
).
In these situations, escape locomotor performance can determine both evasion
of the first predator strike and whether predators abort or give chase
(Webb, 1986
).
Ecological implications
The results of our study indicate that turbidity affected both the
probability of juvenile cod detecting predators with enough time to respond,
and the locomotor performance of their escapes. These effects depended upon
predator attack speed: fish were more likely to evade a fast predator attack
in clear water and a slow predator attack in intermediate turbidity.
The increased probability of capture by fast predators in turbid water
indicates that faster attacks on prey in turbid water are less likely to
elicit an early or fast prey response. Although these results suggest that
predators may increase attack speeds in high turbidity, there are likely to be
sensory-motor limits to this potential strategy. A recent study attributed
reduced attack speeds of a planktivorous fish species in turbid water to less
visual information (Park and Park,
2005
), but we are aware of no studies on the effect of turbidity
on attack speeds of piscivorous fish. If attack speeds of piscivorous
predators in turbid water are limited by sensory-motor constraints, then
turbidity may have a stronger effect on attack rates than capture rates.
Our results suggest that the effects of turbidity on piscivorous
predatorprey interactions are complex and depend on more than reactive
distances or encounter rates (e.g. Miner
and Stein, 1996
; Abrahams and
Kattenfeld, 1997
). Knowledge of predator attack speed, and of prey
evasive performance and behaviour, is also important. The probability of prey
escaping may also be related to the searching speed of the predator, i.e. prey
may be more likely to escape predators that are swimming slowly. Conversely,
predators using faster searching speeds in turbid water may both maximise prey
encounter (e.g. Sweka and Hartman,
2001
) and reduce the probability of eliciting an early or fast
escape response.
Mechano-reception is also used by fish to detect approaching predators
(e.g. Bleckmann et al., 1996
)
and may increase in importance in turbid water [i.e. sensory compensation
(Hartman and Abrahams, 2000
)].
Hence, the outcome of predatorprey interactions in turbid water depends
on the relative sensory abilities of both predator and prey, both in terms of
vision and other sensory modalities
(Vandenbyllaardt et al., 1991
)
(for a review, see Fuiman and Magurran,
1994
). When considering multiple sensory modalities, asymmetries
in predatorprey interactions are likely to be complex as information is
integrated over different spatial and temporal scales by predators and prey
(New et al., 2001
;
Montgomery et al., 2002
).
This study has shown that even a small increase in turbidity can have a
significant effect on visually mediated escape performance of juvenile cod.
Escape performance to a fast predator attack was reduced at a turbidity level
of 3 m1, which corresponds to summer algal blooms in coastal
Norwegian waters and Baltic waters (Hamre
et al., 2003
; Kratzer et al.,
2003
). Cod in deeper waters or in waters with less surface
irradiance are likely to be affected by even lower turbidity levels
(Aksnes and Giske, 1993
). This
suggests turbidity may have an important role in regulating predation
mortality in cod and indicates that further field-based investigation is
required.
| List of symbols and abbreviations |
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| Acknowledgments |
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