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The Journal of Neuroscience, July 1, 2002, 22(13):5727-5733
Thermotaxis in Caenorhabditis elegans Analyzed by
Measuring Responses to Defined Thermal Stimuli
William S.
Ryu and
Aravinthan D. T.
Samuel
Department of Molecular and Cellular Biology, Harvard University,
Cambridge, Massachusetts 02138, and Rowland Institute for Science,
Cambridge, Massachusetts 02142
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ABSTRACT |
In a spatial thermal gradient, Caenorhabditis
elegans migrates toward and then isothermally tracks near its
cultivation temperature. A current model for thermotactic behavior
involves a thermophilic drive (involving the neurons AFD and AIY) and
cryophilic drive (involving the neuron AIZ) that balance at the
cultivation temperature. Here, we analyze the movements of individual
worms responding to defined thermal gradients. We found evidence for a
mechanism for migration down thermal gradients that is active at
temperatures above the cultivation temperature, and a mechanism for
isothermal tracking that is active near the cultivation temperature.
However, we found no evidence for a mechanism for migration up thermal gradients at temperatures below the cultivation temperature that might
have supported the model of opposing drives. The mechanisms for
migration down gradients and isothermal tracking control the worm's
movements in different manners. Migration down gradients works by
shortening (lengthening) the duration of forward movement in response
to positive (negative) temperature changes. Isothermal tracking works
by orienting persistent forward movement to offset temperature changes.
We believe preference for the cultivation temperature is not at the
balance between two drives. Instead, the worm activates the mechanism
for isothermal tracking near the cultivation temperature and
inactivates the mechanism for migration down gradients near or below
the cultivation temperature. Inactivation of the mechanism for
migration down gradients near or below the cultivation temperature
requires the neurons AFD and AIY.
Key words:
thermotaxis; nematode; sensorimotor integration; thermosensation; behavioral models; navigation
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INTRODUCTION |
In their classic study of
thermotaxis in Caenorhabditis elegans, Hedgecock and Russell
(1975) demonstrated that worms navigating spatial thermal gradients
aggregate near their cultivation temperature (Tc). Within 3°C of this
temperature, worms track isotherms, deviating from a given isotherm by
as little as ~0.05°C. Hedgecock and Russell (1975) also harvested
mutants that failed to aggregate at Tc
and found that they could be classified as thermophilic (aggregating in
warmer regions of a plate), cryophilic (aggregating in colder regions
of a plate), or atactic (not aggregating at all). On the basis of this
classification, Hedgecock and Russell (1975) suggested that competing
thermophilic and cryophilic drives produce thermotactic behavior and
that isothermal tracking occurs at their balance.
Mori and Ohshima (1995) identified neurons involved in thermotaxis by
laser ablation. The resulting defects in behavior could be organized in
the same manner as the mutant behaviors shown by Hedgecock and Russell
(1975) , namely thermophilic (obtained by lesion of the AIZ
neuron), cryophilic (obtained by lesion of the AFD and/or
AIY neuron), or atactic (obtained by lesion of the RIA
neuron or multiple neurons). Thus, Mori and Ohshima (1995) proposed
that the AFD and AIY neurons comprise the thermophilic drive, AIZ
comprises the cryophilic drive, and RIA compares the two drives.
Although the labels thermophilic, cryophilic, and atactic describe
aberrant aggregation patterns on spatial gradients, they do not explain
how putative thermophilic and cryophilic drives direct the worm's
movements toward the cultivation temperature. Also, it is unclear
whether thermophilic and cryophilic drives are active during isothermal
tracking or whether isothermal tracking represents a distinct mechanism.
The present study aimed to determine the mechanisms underlying
thermotaxis, the manner in which they direct the worm's movements, and
the roles of participating neurons. We studied the movements of worms
as they performed thermotaxis by (1) tracking worms crawling on the
surface of agar plates with defined spatial or temporal thermal
gradients and (2) monitoring the swimming motions of a worm suspended
in a droplet subjected to thermal stimuli. In addition to wild-type
(N2) worms, we studied thermotaxis mutants that have been shown to have
developmental defects in AFD or AIY neurons, which have been identified
by Mori and Ohshima (1995) to be involved in thermotaxis.
We found strong evidence for a mechanism for migration down gradients
toward the cultivation temperature that might correspond to the
cryophilic drive of the prevailing model, but no compelling evidence
for a mechanism for migration up gradients that might correspond to the
thermophilic drive. The mechanism for migration down gradients
modulates run duration but not run orientation, shortening runs in
response to positive changes in temperature and lengthening runs in
response to negative changes in temperature. The mechanism for
isothermal tracking modulates run orientation to offset either positive
or negative temperature changes. These data (the asymmetry between
navigation above and below the cultivation temperatures and the
different nature of the motor commands between migration down gradients
and isothermal tracking) seem to undermine the prevailing simple model
of competing cryophilic and thermophilic drives.
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MATERIALS AND METHODS |
Media and strains. C. elegans strains were
grown and maintained as described by Sulston and Hodgkin (1988) (N2 was
a gift from Craig Hunter, Harvard University, Cambridge, MA).
The mutants ttx-3 (ks5) and ttx-1(p767) were
obtained from Theresa Stiernagle at the C. elegans Genetic
Center (University of Minnesota, Minneapolis, MN).
Thermal gradients on surfaces. Linear thermal gradients were
established on agar surfaces by placing Petri dishes in the middle of
rectangular aluminum plates, the ends of which were fixed at different
temperatures. Glycerol was used to ensure good thermal contact between
the Petri dish and the metal surface. In one apparatus, thermoelectric
controllers (TECs) were fixed to the ends of an aluminum plate (5 × 12.7 × 0.32 cm). The TECs (3 cm square, 50 W) were
thermostatically controlled to 0.1°C with a linear-bipolar Proportional Command Integral Control controller (HTC-3000;
Wavelength Electronics, Bozeman, MT). With this apparatus,
arbitrary gradients (as steep as 5°C/cm) could be programmed. An
apparatus of the type used by Hedgecock and Russell (1975) was also
built. In this case, a linear gradient was established along a 60 × 10 × 1.3 cm aluminum plate by bolting 10 × 10 × 6 cm blocks to each end, immersing one block in a thermostatically
controlled water bath, and immersing the other in an ice bath. The
temperature at the agar surface was measured with a T-type thermocouple
(0.1°C resolution). The agar plates reached thermal equilibrium
within 10 min. Gradients were linear up to 1 cm from the edge of the
Petri dish.
The choice of temperatures for cultivating and testing worms was not
arbitrary. Worms cultivate well in the range 15-25°C (Sulston and
Hodgkin, 1988 ). At temperatures <15°C, worms become lethargic. We
did not test worms at temperatures >27°C to avoid eliciting
heat-shock or pain responses (Wittenburg and Baumeister, 1999 ). Also,
the temperature range for thermotaxis assays has traditionally been
from 17 to 25°C in radial thermal gradients, and we sought comparable conditions.
Temporal thermal ramps were produced by controlling the temperature of
a brass plate (11 cm in diameter, 0.32 cm thick) in contact with a TEC.
Plates (9 cm) containing nematode growth medium (NGM) (Sulston and
Hodgkin, 1988 ) were sealed to the brass plate with a thin layer of
glycerol. Spatial temperature variation along the agar surface was
negligible. Temperatures were stable to 0.1°C, and ramping rates up
to 10°C/min could be achieved. In all temporal ramping experiments,
we used the rate of 0.5°C/min. Ramp duration was 5 min and was linear
for the middle 3 min. Worms were tracked only during the linear portion
of the ramps.
All experiments were done in a temperature-controlled room set to a
temperature between the limiting temperatures of the gradient. For
example, for a gradient between 17 and 19°C, the room temperature was
set to 18 ± 0.1°C. The numbers of worms analyzed in each
experiment are listed in the figure legends.
Thermal gradients in droplets. Temporal thermal ramps in
droplets were produced by controlling the temperature of an anodized aluminum plate (43 × 48 × 5 mm) in contact with a TEC. NGM
buffer (60 µl; same inorganic ion concentration as NGM plates) was
placed in a 4 mm circular hole in the plate, forming a transparent,
hanging droplet. Temperatures were stable to 0.1°C; ramping rates up
to 20°C/min could be achieved.
Crawling assays. Populations were synchronized by selecting
eggs to OP50-seeded NGM plates (Sulston and Hodgkin, 1988 ).
These plates were incubated at specific temperatures between 15 and 25°C. We monitored incubator temperatures for constancy
(Tc of ±0.1°C). Immediately before
each assay, ~20 young adult worms were washed in 10 ml of NGM buffer
at room temperature (same inorganic ion concentration as NGM plates)
and moved to fresh NGM plates without bacteria. These plates
were then placed on the metal surface of the equipment described above.
A glass cover on the NGM plate was used during assays to eliminate
variations in humidity, temperature changes attributable to evaporative
cooling, and air currents.
A CCD camera (wv-BP550; Panasonic, Secaucus, NJ) equipped with a
9-27 mm zoom lens (f/2.0) was used to image the worms. Worms were
illuminated obliquely by a ring of superbright red light-emitting diodes, producing a dark-type illumination. Magnification was set such that the Petri dish filled the field of view. Video images were captured at 1 frame per second (fps) by a Scion Image LG-3 capture
board (Scion Corp., Frederick, MD) on either a Macintosh computer
(PowerMac G3; Apple Computers, Cupertino, CA) or a personal computer
(Pentium III; Dell Computer Company, Round Rock, TX).
For the spatial assays, worms at a specific cultivation temperature
were prepared as described above. A glass plate was used to cover the
Petri dish to reduce convection. After waiting 15 min to ensure that
the worms and plate had reached thermal equilibrium, video images of
the plate were captured for 500 sec at 1 fps.
For the temporal assays, we waited for 1 min after the onset of the
ramp before capturing images. During the subsequent linear part of the
ramp, images were captured for 120 sec at 1 fps.
Worm trajectories were scored by hand using the imaging program Scion
Image (Scion Corp.) Worm paths within 1 cm of the plate edge were not
scored to avoid artifacts arising from thermal edge effects. Numerical
analysis was performed with conventional and customized algorithms
using Matlab (MathWorks Inc., Natick, MA).
Swimming assays. Worms cultivated at specific temperatures
were prepared as described above; single worms were placed in the droplet. Worms were imaged using a stereomicroscope and a CCD camera.
Worms swam vigorously, but sinking to the bottom of the curved droplet,
they stayed in the center of the field of view. Bends that terminated
the swimming run were scored by eye. We did not sort large bends
based on the degree or direction of bending. For swimming worms, we did
not score reversals of the direction of wave propagation; reversals
were rare, and they did not contribute significantly to the statistics
of run termination.
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RESULTS |
Migration toward cultivation temperature
Worms swim through fluids or crawl on surfaces using snake-like
movements. We define a run as a period of uninterrupted forward motion
(either swimming or crawling) in which bending waves propagate continuously from nose to tail. Crawling and swimming worms terminate runs in analogous manners: crawling worms terminate runs by abrupt reorientations that might be either turns or pirouettes (Fig. 1); swimming worms terminate runs by
abrupt bends larger than those of the forward swimming rhythm (Fig. 1)
or by reversing the direction of wave propagation. See Croll (1975) for
an early behavioral study that connects abrupt bends of swimming worms with the abrupt reorientations of crawling worms.

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Figure 1.
Run termination in crawling and swimming worms.
Crawling worms terminate runs by turns (a) or by
pirouettes (b), which involve reversals and
coiling. c, Swimming worms terminate runs by abrupt
bends larger than those of the rhythmic bends of forward
swimming.
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To determine whether worms modulate the run duration in response to
thermal stimuli, we measured run durations of worms exposed to rising
and falling temperatures (ramps). In assessing the run duration of
crawling worms, we scored both turns and pirouettes, because both
terminate the previous run and choose a new orientation for the
subsequent run. In assessing the run duration of swimming worms, we
scored the frequency of large bends.
In assays of crawling worms, we ramped the temperature of entire
plates, eliminating spatial gradients. We found that above Tc, the run durations in negative
temporal gradients (i.e., falling temperatures) were lengthened,
whereas the run durations in positive temporal gradients (i.e., rising
temperatures) were shortened compared with the run durations in
isotropic environments at temperatures within the range of the temporal
ramps (Tables 1 and
2). Below Tc, run durations were the same
regardless of whether the temperature rose or fell (Table 2). Run
durations were exponentially distributed, suggesting Poisson statistics
(Fig. 2). The rate of run termination in
isotropic environments, attributable to background activity not evoked
by temperature changes, rose monotonically with ambient temperature and
by itself cannot drive aggregation at
Tc (Table 1).
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Table 1.
Run durations of N2 worms cultivated at different
temperatures crawling on agar surfaces at fixed temperatures (i.e.,
without temporal or spatial variation)
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Table 2.
Run durations of N2 worms cultivated at different
temperatures crawling on agar surfaces subjected to temporal ramps
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Figure 2.
A sample histogram of run durations of N2 worms
crawling in an isotropic environment (21°C). The data shown
correspond to ~150 runs of worms raised at 22°C; the mean of this
distribution corresponds to an entry in Table 1. The distribution is
fit by a single exponential line: run termination might be a
first-order kinetic process obeying Poisson statistics. The histogram
was binned with 10 sec width.
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In assays of swimming, we ramped the temperature of droplets (60 µl)
containing single worms. Confined to a droplet, a worm made visible
swimming motions but did not leave the field of view. Run termination
events were more frequent for swimming worms than for crawling worms.
We measured the durations of all runs of populations of worms crawling
on plates, and we scored the times of occurrence of run termination
events of individual worms swimming in droplets (Fig.
3). We found that the thermotactic
response for swimming worms was analogous to that of crawling worms.
Above Tc, the number of run
termination events per unit time was lower during negative ramps and
higher during positive ramps compared with measurements using droplets
of a fixed temperature within the range of the temporal ramps. Below
Tc, the rate of run termination was
the same regardless of whether the temperature rose or fell.

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Figure 3.
Times of occurrence of run termination events of
N2 worms cultivated at 20°C swimming in droplets. Experiments at
temperatures below Tc are at the
left, and experiments at temperatures above
Tc are at the right.
Experiments at fixed temperatures are at the top (19°C
for T < Tc;
24°C for T > Tc). Experiments subjecting the drops
to positive temporal ramps of +4°C/min are in the
middle (17-19°C for T < Tc; 22-24°C for
T > Tc).
Experiments subjecting the drops to negative temporal ramps of
4°C/min are at the bottom (19-17°C for
T < Tc;
24-22°C for T > Tc). Within a panel,
individual experimental trials are aligned along the vertical axis. Run
termination events during a trial are indicated by closed
squares; their horizontal positions indicate their times
of occurrence from the beginning of each trial. (In the case of the
ramp experiments, trials begin at the onset of the ramp.) All trials
lasted 30 sec. For T < Tc, the rate of run termination was
0.26 ± 0.04 and 0.33 ± 0.04 Hz for positive and negative
ramps, respectively; for T > Tc, the rate of run termination was
0.56 ± 0.03 and 0.08 ± 0.02 Hz for positive and negative
ramps, respectively. The rate of run termination at fixed temperatures
was 0.33 ± 0.08 and 0.22 ± 0.03 Hz for 19°C and 24°C,
respectively. Values are means ± SEM.
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During runs, worms crawled at the same speed in both positive and
negative temporal ramps (Table 3).
Therefore, controlling run speed is not part of the thermotactic
strategy. Run speed had a much weaker dependence on ambient temperature
than the rate of run termination (compare Tables 1 and 3).
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Table 3.
Run speeds of N2 worms cultivated at 22°C in isotropic
environments of different temperatures and subjected to temporal ramps
toward or away from 22°C
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In spatial gradients, worms might arrive more quickly at
Tc by biasing reorientation or run
curvature toward Tc rather than by
picking run direction and curvature randomly. To address this issue, we
studied the trajectories of worms migrating toward
Tc on the surfaces of agar plates with
spatial thermal gradients. On spatial gradients in which worms rapidly
migrated down gradients toward Tc,
abrupt reorientations did not direct worms toward the favorable
direction (Fig. 4a), nor did
worms steer by gradually turning toward
Tc (Fig. 4b).

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Figure 4.
a, Initial and final run
orientations interrupted by single abrupt reorientations
(n = 413). Here, N2 worms cultivated at 22°C
navigated a linear spatial gradient between 24 and 26°C of steepness
0.4°C/cm. The direction down the gradient was 0 radians. Final run
orientations were not more clustered at 0 radians than initial run
orientations, as would be the case if the angle of abrupt reorientation
was not random and angle selection was weighted toward the favorable
direction of movement. Along both axes there is a greater frequency of
events between  /2 and + /2 radians, but this is an
artifact: only abrupt reorientations in which both initial and final
runs were longer than approximately three body lengths were used. This
criterion enabled accurate measurement of run orientation, but on such
steep gradients also reduced events corresponding to run orientations
less than  /2 or greater than + /2. However, the relevant feature
of this plot that survives this artifact is that the dispersion around
0 radians, the desired direction, is apparently the same for the final
as for the initial run orientations. A numerical analysis of this data
set shows that the rms deviations from 0 radians for the initial and
final run orientations are 1.4 radians and 1.5 radians, respectively:
worms are not better oriented toward 0 radians after abrupt
reorientations. Similar results were obtained for worms cultivated at
22°C and navigating gradients between 17 and 19°C (data not shown).
b, Traces of runs of duration of ~20 sec. Here, N2
worms cultivated at 22°C navigated a linear spatial gradient between
24 and 26°C of steepness 0.4°C/cm, a steepness at which worms
robustly migrated down gradients but did not always terminate runs
within a few seconds when moving up gradients. Forpresentation purposes, we have centered all runs as
emerging from a single point. The arrow indicates the
direction down the gradient. More tracks are to the
right (n = 27) than to the
left (n = 15), but the essential
data are the shape and not the number of the tracks. The number of
tracks to the right is larger because in any trial there
were more runs of 20 sec duration down the gradient than up the
gradient attributable to the worm's strategy of shortening or
lengthening runs up or down the gradient. Based on the shape of the
individual tracks, we conclude that worms did not steer individual runs
toward the direction of the gradient. Some runs were curved, but the
curvature was randomly CW or CCW and was not correlated with the
gradient. Similar results were obtained for worms cultivated at 22°C
and navigating gradients between 17 and 19°C (data not shown).
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In our hands, when navigating even the steepest spatial gradients
(4°C/cm) at temperatures below Tc,
worms did not actively migrate toward
Tc. Neither the run duration nor the
run orientation was modulated to bias the worms up (or down) the
gradients. Worms navigating at temperatures below
Tc are atactic. Worms were able to
aggregate near Tc by tracking
isotherms on random arrival near Tc,
but if they have a strategy for active migration up gradients toward
Tc, it is undetectably weak using our assays.
In summary, when migrating toward Tc,
worms modulate run duration but do not modulate run speed or
orientation. When worms navigate at temperatures above
Tc, they modulate the frequency of
abrupt reorientations to migrate down the gradient: worms terminate runs more rapidly when moving away from
Tc than when moving toward Tc. However, worms do not choose the
angle of abrupt reorientations to direct runs in the more favorable
direction. In contrast, when worms navigate at temperatures below
Tc, we found no compelling evidence of
a mechanism for migration up gradients toward higher temperatures.
Isothermal tracking
Worms crawling on a spatial thermal gradient track isotherms near
Tc. On linear spatial gradients, they
move along lines; on radial spatial gradients, they move in circles
(Hedgecock and Russell, 1975 ; Mori and Ohshima, 1995 ). Hedgecock and
Russell (1975) found that individual tracks are narrow (~0.05°C)
but could occur as far as 3°C from
Tc. A worm can track an isotherm in
either direction, keeping the higher temperature to its left or its right.
We measured the trajectories of isothermal tracks on linear spatial
gradients of varying steepness (Fig. 5).
Worms zigzagged along isothermal tracks (i.e., when they crawled too
far from the targeted isotherm, they turned back toward it). The
frequency of the zigzag increased and the width of the zigzag decreased on steeper thermal gradients (Fig. 5b,c). Whatever the
gradient steepness, worms responded by turning when they arrived at the temperature boundaries of the targeted isotherm. These boundaries were
within ~0.05°C of that isotherm.

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Figure 5.
a, A single isothermal track of an
N2 worm cultivated at 22°C on a linear thermal gradient of steepness
0.4°C/cm. b, Isothermal tracks were narrower as the
steepness of thermal gradients increased. One metric of the
width of isothermal tracks is
y2 1/2, the
mean square deviation from the midline of the track. Here, excursion
amplitude is defined as the mean
y2 1/2 of ~50
isothermal tracks of N2 worms cultivated at 22°C on three different
gradients (0.4, 0.75, and 2°C/cm). Note that the metric of
y2 1/2 (i.e., 1 SD)
is not the overall side-to-side width of a track. A better estimate is
4 y2 1/2, which
corresponds to the width in which the worm spends 95% of its time
during a track. The corresponding temperature boundaries of isothermal
tracks (the product of gradient steepness and
4 y2 1/2) is 0.1 ± 0.01°C. c, In steeper gradients, the frequency of
the side-to-side movement increased. Here, we show the normalized power
spectrums of the isothermal tracks described in Figure
4b.
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As found by Hedgecock and Russell (1975) , worms tracked isotherms
far from Tc (Fig.
6a). A single worm can track
multiple isotherms. The movement of one such worm, which left one
isotherm and resumed tracking on a parallel isotherm at a
different temperature, is shown in Figure 6b. The
distribution of temperatures at which a worm might track an isotherm is
far broader than the width of a single isotherm. This is evidence that
thermal preference is represented by the distribution of temperatures
at which a worm might track isotherms, and not the temperature of any
particular isotherm. Moreover, this distribution is not always centered
on Tc (Fig. 6a). However,
the observation pertinent to the present argument is that the width of
the distribution is ~20-30 times broader than the width of a single
track.

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Figure 6.
a, N2 worms cultivated at 22°C
tracked isotherms in a range within 2°C of that cultivation
temperature. The histogram shows the positions of the isotherms of
~40 worms drawn from a single plate tracked on a linear thermal
gradient of steepness 0.4°C/cm and binned at a width of 0.4°C.
b, Individual worms often stopped tracking one isotherm
and resumed tracking a different one. This trace is an unusually clear
example: the worm initially tracked at 21°C, fell off the isotherm,
and continued to track at 22°C.
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We suggest that isothermal tracking represents a behavioral mechanism
that is active within a band of temperatures near
Tc, and that it is not derived from
the worm's behaviors when navigating at temperatures above or below
Tc. Worms, when navigating at
temperatures near Tc, track isotherms
by avoiding temporal changes in temperature, turning to offset any
changes exceeding ~0.05°C. In this case, as we have observed, a
worm deviating from an isothermal track in steeper gradients would
react more quickly (higher zigzag frequency) and within a shorter
distance (smaller zigzag width). We suggest that the decision whether
to track isotherms depends on the worm's comparison of the ambient
temperature with Tc; the decision is yes if the worm is within 2-3°C of
Tc.
Analysis of mutants
To determine the roles of individual neurons in the identified
thermal circuit, we analyzed worms lacking AFD or AIY because of the
developmental mutations ttx-1 (Satterlee et al., 2001 ) and
ttx-3 (Hobert et al., 1997 ). The mutation ttx-1
is thought to be specific to the AFD neuron. Although the mutation
ttx-3 is not specific to AIY, the other neurons it affects
are outside the known thermotaxis circuit. Previous workers have
characterized both ttx-1 and ttx-3 as defective
in thermotaxis; we hoped that their defects would shed light on the
wild-type mechanisms that comprise thermotaxis (see above).
Worms that lack AIY are cryophilic and do not track isotherms (Mori and
Ohshima, 1995 ; Hobert et al., 1997 ). We found that the mechanism for
migration down gradients toward lower temperatures that modulates run
duration is constitutively active in worms lacking AIY because of the
mutation ttx-3 (Table 4). The
mechanism for migration down gradients controls the movements of
wild-type worms only at temperatures above
Tc but controls the movements of
ttx-3 worms at all temperatures. It has come to our
attention that stronger alleles than ttx-3 have been
isolated, but the phenotype of the mutant we analyzed, ttx-3
(ks5), is robust in our assays and fully penetrant (affecting
100% of worms).
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Table 4.
Run durations of N2 and ttx-3 (ks5) worms
navigating isotropic environments and subjected to temporal ramps
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Laser ablation of AFD produces cryophilic or atactic worms (Mori and
Ohshima, 1995 ). As we found for worms lacking AIY, worms lacking AFD
because of the mutation ttx-1 (Satterlee et al., 2001 ) have
a constitutively active mechanism for migration down gradients toward
lower temperatures (data not shown). More strikingly, however, ttx-1 worms crawling on the surfaces of agar plates usually
moved in clockwise (CW) or counterclockwise (CCW) circles (Fig.
7). Circling was independent of ambient
temperature, presence of spatial or temporal thermal gradients, or
Tc. Circling was not observed on
cultivation plates in which worms crawl through bacterial lawns. Therefore, circling represents a defect in taxis, not a defect in
locomotion, and suggests a flaw in a mechanism that normally controls
the direction of turning or run orientation.

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Figure 7.
Trajectories of crawling ttx-1
worms. Circling is either CW or CCW and is independent of ambient
temperature or spatial gradients.
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DISCUSSION |
Our results do not easily reconcile with current opinion that
thermotaxis is a balance between separate thermophilic and cryophilic drives (Thomas, 1995 ; Mori and Ohshima, 1997 ; Mori, 1999 ). Instead, we
suggest that thermotaxis involves two mechanisms: (1) a mechanism for
tracking isotherms and (2) a mechanism for migration down gradients
toward lower temperatures. In wild-type thermotaxis, we found no
evidence for a mechanism for migration up gradients toward higher temperatures.
Both mechanisms for tracking isotherms and for migration down gradients
toward lower temperature respond to positive and negative changes in
temperature, but the two mechanisms are active in different temperature
regimes and control the worm's movements in different manners. The
mechanism for isothermal tracking is active at temperatures near
Tc. This mechanism controls run
orientation, responding to positive and negative changes in
temperature by prompting turns to offset the changes. The mechanism for
migration down gradients toward lower temperatures is active at
temperatures above Tc. This mechanism
controls run duration but not run orientation, responding to positive
or negative changes in temperature by shortening or lengthening runs.
A calcium-binding protein, expressed in AFD, AIY, and other neurons, is
essential for isothermal tracking (Gomez et al., 2001 ). Laser ablation
of AFD or AIY abolishes isothermal tracking (Mori and Ohshima, 1995 ).
We found that mutant worms with a developmental defect in AFD have a
defect in turning that might indicate a flawed mechanism for isothermal
tracking, because this mechanism normally controls turns and turn
angles. Together, these results suggest that the mechanism for
isothermal tracking includes AFD and AIY.
In mutants with developmental defects in AFD or AIY, the mechanism for
migration down gradients toward lower temperatures is active at all
temperatures irrespective of Tc. We
suggest that the mechanism for isothermal tracking (involving AFD and
AIY) is needed to suppress the mechanism for migration down gradients at temperatures near or below Tc. We
do not know which neurons comprise the mechanism for migration down
gradients toward lower temperatures.
Pierce-Shimomura et al. (1999) studied chemotaxis by tracking worms on
defined salt gradients. Their results are similar to ours for migration
down gradients toward lower temperatures. In both mechanisms for
migration on chemical gradients and migration down thermal gradients,
worms initiate abrupt reorientations to terminate runs that carry them
away from their target. This shared feature suggests that the
mechanisms for migration on chemical gradients and migration down
thermal gradients might have other similarities (e.g., parallel
connections to the same motor neurons).
Others have reported both thermophilic and cryophilic phenotypes
attributable to mutation or laser ablation (Hedgecock and Russell,
1975 ; Mori and Ohshima, 1995 ). Thermophilia has been explained as
damage to the cryophilic drive; cryophilia has been explained as damage
to the thermophilic drive. However, after considering the mechanisms
that underlie normal thermotaxis, these explanations no longer seem
adequate. Cryophilia, like that of mutants lacking AFD or AIY, can be
explained by constitutive activity of the mechanism for migration down
gradients. However, because normal thermotaxis does not exhibit a
mechanism for migration up gradients, there is no similar alteration of
the normal mechanisms of thermotaxis that might explain thermophilia.
It is possible to speculate about more subtle alterations of the two
normal mechanisms that underlying thermotaxis that might cause worms to
aggregate at temperatures higher than
Tc. For instance, worms might add a
constant offset to their memory of Tc,
and thus may track isotherms (and thus aggregate) at temperatures
warmer than the true Tc.
Also, the worm's preference for Tc
has been explained as the balance between thermophilia and cryophilia.
This explanation is also no longer adequate. Isothermal tracking
reflects a capacity to compare ambient temperature with
Tc: worms have a long-term memory of
Tc; they track any isotherm near
Tc. While tracking isotherms, worms
react to small temperature changes by modulating run orientation,
turning to offset these changes. In our view, the worm's behavior near
Tc is not derivative of its behaviors above and below Tc. The behavior near
Tc is qualitatively different from its
behaviors above and below Tc: above
Tc, the worm modulates run duration
and not run orientation to migrate down gradients; below
Tc, there is no active thermotactic mechanism.
Long-term memory of Tc determines the
regimes of activity of the mechanisms for tracking isotherms and
migration down gradients. Both mechanisms appear to make short-term
comparisons of temperature, enabling responses to positive and negative
temperature changes. However, these mechanisms control the worms'
movements in different manners, the mechanism for migration down
gradients controls only run duration; the mechanism for tracking
isotherms controls run orientation. Elucidating the relationships
between these two mechanisms, determining their shared and distinct
neural circuit elements, and determining which neuron(s) are the
primary transducers of temperature (specifically which neurons compare
ambient temperature with a long-term memory of
Tc and which neurons make short-term comparisons of temperature) are future goals uncovered by the present work.
 |
FOOTNOTES |
Received Nov. 27, 2001; revised April 3, 2002; accepted April 15, 2002.
This work was supported by the Rowland Institute for Science. The
C. elegans Genetics Center, a facility supported by
the National Institutes of Health, provided mutant strains. A.D.T.S. is
an Amgen Fellow of the Life Sciences Research Foundation. We thank
Venkatesh Murthy and Howard Berg, and members of their laboratories, for useful discussions, sharing resources, and critical reading of this
manuscript. We thank an anonymous reviewer for critical comments.
Correspondence should be addressed to Dr. Aravinthan Samuel, Cold
Spring Harbor Laboratories, 1 Bungtown Road, Cold Spring Harbor, NY
11724. E-mail: samuel{at}cshl.org.
 |
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