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The Journal of Neurophysiology Vol. 88 No. 2 August 2002, pp. 914-928
Copyright ©2002 by the American Physiological Society
1Department of Otolaryngology, Tokyo Women's Medical University Daini Hospital, Tokyo 116-8567, Japan; 2Department of Neurology, Mount Sinai School of Medicine, New York, New York 10029-6574; 3Department of Otolaryngology, Teikyo University School of Medicine, Tokyo 173-8605, Japan; and 4Department of Computer and Information Science, Brooklyn College, City University of New York, Brooklyn, New York 11210
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ABSTRACT |
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Arai, Yasuko,
Sergei
B. Yakushin,
Bernard Cohen,
Jun-Ichi Suzuki, and
Theodore Raphan.
Spatial Orientation of Caloric Nystagmus in Semicircular
Canal-Plugged Monkeys.
J. Neurophysiol. 88: 914-928, 2002.
We studied caloric nystagmus before and after plugging
all six semicircular canals to determine whether velocity storage
contributed to the spatial orientation of caloric nystagmus. Monkeys
were stimulated unilaterally with cold (
20°C) water while upright, supine, prone, right-side down, and left-side down. The decline in the
slow phase velocity vector was determined over the last 37% of
the nystagmus, at a time when the response was largely due to
activation of velocity storage. Before plugging, yaw components varied
with the convective flow of endolymph in the lateral canals in
all head orientations. Plugging blocked endolymph flow, eliminating convection currents. Despite this, caloric nystagmus was readily elicited, but the horizontal component was always toward the stimulated (ipsilateral) side, regardless of head position relative to gravity. When upright, the slow phase velocity vector was close to the yaw and
spatial vertical axes. Roll components became stronger in supine and
prone positions, and vertical components were enhanced in side down
positions. In each case, this brought the velocity vectors toward
alignment with the spatial vertical. Consistent with principles
governing the orientation of velocity storage, when the yaw component
of the velocity vector was positive, the cross-coupled pitch or roll
components brought the vector upward in space. Conversely, when yaw eye
velocity vector was downward in the head coordinate frame, i.e.,
negative, pitch and roll were downward in space. The data could
not be modeled simply by a reduction in activity in the ipsilateral
vestibular nerve, which would direct the velocity vector along the roll
direction. Since there is no cross coupling from roll to yaw,
velocity storage alone could not rotate the vector to fit the data. We
postulated, therefore, that cooling had caused contraction of the
endolymph in the plugged canals. This contraction would deflect the
cupula toward the plug, simulating ampullofugal flow of endolymph.
Inhibition and excitation induced by such cupula deflection fit the
data well in the upright position but not in lateral or prone/supine
conditions. Data fits in these positions required the addition of a
spatially orientated, velocity storage component. We conclude,
therefore, that three factors produce cold caloric nystagmus after
canal plugging: inhibition of activity in ampullary nerves, contraction
of endolymph in the stimulated canals, and orientation of eye velocity
to gravity through velocity storage. Although the response to
convection currents dominates the normal response to caloric
stimulation, velocity storage probably also contributes to the
orientation of eye velocity.
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INTRODUCTION |
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Thirty years after the discovery
that the sense of angular motion was due to activation of the
semicircular canals (Breuer 1874
; Crum-Brown
1874
; Mach 1875
), and shortly after Ewald
(Ewald 1892
) established the physiological mechanism of
canal activation using a "pneumatic hammer" and canal plugging,
Robert Bárány discovered that nystagmus could be induced by
irrigation of the external auditory canals with cold or warm water
(Bárány 1906
). With the head tilted up 30°
from the supine so that the lateral canal planes are aligned with the
spatial vertical, introduction of cold water into one ear induces
horizontal nystagmus with ipsilateral slow phases, presumably coming
predominantly from the ipsilateral lateral canal. Irrigation with warm
water produces an oppositely directed nystagmus. If the head is placed
30° down from the prone position, the lateral canal is inverted in
space from the supine position, and the nystagmus produced by cold and
warm stimuli reverses direction. From this, Bárány inferred
that the induced nystagmus was the result of utriculopetal or
utriculofugal deflection of the cupula in the lateral canals caused by
convection currents, which were produced by local cooling or warming of
the endolymph moving toward or away from gravity. This resulted in the
caloric test, which almost 100 yr later, is still widely used
clinically to determine and compare the response of the lateral
semicircular canals.
Other factors could also contribute to the caloric response. Direct
cooling or warming of the nerves increases or decreases firing rates in
the vestibular nerve (Klinke 1992
). This is likely to be
responsible for the differences in caloric response in the supine and
prone positions, in which the induced horizontal eye velocity from cold
caloric stimulation is greater in face-up than face-down positions
(Clarke et al. 1988
; Coats and Smith
1967
; Hood 1989
; Minor and Goldberg
1990
; Paige 1985
). It has been estimated that
about 75% of the caloric response is the result of convection currents, and about 25-30% of the response is due to warming or cooling of the nerve (Minor and Goldberg 1990
).
Additionally, since the caloric response is due to stimulation of the
semicircular canals, such stimulation should cause activation of
central circuits responsible for velocity storage. Velocity storage,
which is activated by vestibular, visual, and somatosensory inputs,
improves the low frequency characteristics of the angular
vestibulo-ocular reflex, sustains eye velocity during prolonged
rotation of the subject or the visual surround, and counters vestibular
after-responses (Cohen et al. 1977
; Raphan et al.
1979
; see Raphan and Cohen 1996
, 2002
for review).
A striking feature of velocity storage is its spatial orientation. In
the monkey, the duration and gain of the yaw, pitch, and roll
components of vestibular and optokinetic nystagmus are altered so that
they tend to maintain the eye velocity vector of the nystagmus aligned
with gravity or with gravito-inertial acceleration (GIA), the sum of
the linear accelerations acting on the head (Dai et al.
1991
; Raphan and Sturm 1991
; Wearne et al. 1996
-1999
). The yaw time constant is longest, and the
pitch and roll time constants are shortest in the upright position, when the velocity vector of the induced nystagmus is coincident with
the earth-vertical, i.e., with gravity (Dai et al.
1991
). In side down or prone and supine positions, the time
constants of the pitch and roll components, respectively, are maximal,
and the yaw axis time constant is reduced (Dai et al.
1991
). Pitch and roll eye velocities also appear when yaw axis
nystagmus is induced with the head in tilted positions. These
velocities arise because of cross-coupling of activity from yaw to
pitch or roll. An important assumption in modeling the orientation
properties of velocity storage is that there is no cross-coupling from
pitch or roll to yaw (Dai et al. 1991
; Raphan and
Sturm 1991
; see Raphan and Cohen 1996
for review).
Because the convection currents that are produced by segmental cooling
or warming of the endolymph are oriented with respect to gravity
(Bárány 1906
), it has been difficult to
determine whether the orientation properties of velocity storage
contribute to the response. This is primarily because the convection
currents in the lateral canals produced by cooling or warming the
endolymph are also oriented to gravity and overwhelm other
contributions (Aw et al. 1998
; Böhmer et
al. 1992
, 1995
). A number of studies have demonstrated unknown,
nonconvective mechanisms that could tend to orient eye velocity toward
gravity (Böhmer et al. 1995
; Fetter et al.
1998
; Paige 1985
; Stahle
1990
; Yagi et al. 1992
), but there is
little information about the degree to which velocity storage might be
involved (Arai et al. 1989
, 1998
; Kawachi
1992
; Tshuchiya 1995
). Two lines of evidence
suggest that velocity storage is activated by caloric stimulation. If
caloric nystagmus is suppressed by exposure to a stationary visual
surround during its early phases, slow phase velocity recovers slowly,
suggesting reactivation of central circuits by afferent input
(Raphan and Cohen 1981
; Takemori and Cohen
1974
). Moreover, if caloric nystagmus is suppressed by light in
its terminal stages, eye velocity never recovers, presumably because
cupula deflection has ceased, and the terminal portions of the caloric
response are produced predominantly by central activity from velocity
storage. Both findings have been modeled by a central integrator that
adds to the activity produced by cupula deflection in its early stages
but that outlasts cupula deflection (Raphan and Cohen
1981
).
Elimination of convection currents is one way to study the contribution
of the nonconvective mechanisms, which include velocity storage, to
caloric nystagmus. During a Skylab space flight, where the
gravitational field was reduced to
10
6
g, robust caloric nystagmus was elicited by bithermal
stimulation, despite the absence of convection currents (Clarke
and Scherer 1988
; Scherer and Clarke 1985
,
1987a
,b
; Scherer et al. 1986
). The source of the
response to caloric stimulation in microgravity is not entirely clear,
but Scherer and Clarke proposed that in addition to its effects on the
vestibular nerve, cooling had caused a difference in pressure between
the arm of the canal adjacent to the cupula and the endolymph in the
vestibule on the opposite side of the cupula, producing hair cell
deflection (Clarke et al. 1993a
,b
; Scherer and
Clarke 1985
). How the orientation properties of velocity
storage might contribute to the spatial orientation of the induced
nystagmus could not be inferred from these studies, however, because
the linear acceleration of gravity is so weak in orbital flight.
Another way to eliminate convection and maintain the orientation
properties of velocity storage is to interrupt the flow of endolymph by
plugging the semicircular canals (Ewald 1892
). The end
organs are histologically intact after canal plugging (Angelaki et al. 1996
; Arai et al. 1996
; Camis
1930
; Ewald 1892
; Suzuki et al.
1991
; Yakushin et al. 1998
), the resting
discharge is unaltered in the afferent fibers (Goldberg and
Fernandez 1975
; Rabbitt et al. 1999
), and the
orientation properties of velocity storage are unaltered (Raphan
et al. 1992b
). The canals remain active in detecting angular
acceleration after canal plugging (Lasker et al. 1999
;
Rabbitt et al. 1999
; Yakushin et al.
1998
), but the dominant time constant of the plugged canals is
reduced from 4-5 s (Büttner and Waespe 1981
;
Correia et al. 1992
; Goldberg and Fernandez
1971
; Reisine et al. 1988
) to about 0.07 s
(Yakushin et al. 1998
). As a result, the high-pass
cutoff characteristics of the canals move to considerably higher
values, further reducing the effect of low-frequency stimulation, such
as would occur from convection currents. On the other hand, the
duration of the induced nystagmus has been shown to be approximately
the same in canal-plugged as in normal animals (Arai et al.
2000
). Therefore the duration of the stimulus in the bone must
have been the same, despite the fact that the mastoid had been opened
to reach the inner ear in the canal-plugged animals. Optokinetic
after-nystagmus (OKAN) was also preserved after canal plugging, so that
velocity storage was operative. Canal plugging, therefore, presents a
unique opportunity to study the characteristics of nonconvective
mechanisms and the role of velocity storage in producing the caloric
response in three dimensions.
The purpose of this study was to characterize the orientation properties of caloric nystagmus in canal-plugged animals, which could be compared with the orientation of the nystagmus induced by convection currents and other factors in the intact animal. If velocity storage contributes to caloric nystagmus, then caloric stimulation in the upright position would be expected to produce little or no cross-coupling from yaw to pitch and/or roll, and the pitch and roll components would almost entirely be due to direct activation of the lateral canal and the adjacent anterior canal. In side down, prone, and supine positions, however, there should be substantial cross-coupling of the induced horizontal nystagmus to either pitch or roll, depending on the position of the head with regard to gravity.
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METHODS |
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Experiments were performed on five cynomolgus monkeys. In two,
all six semicircular canals were plugged, and they were tested before
and after operation. The responses to rotation before and after
operation in these animals have been reported in detail elsewhere
(Yakushin et al. 1998
). Three other animals with intact canals were used as controls. The data from the canal-plugged animals
form the basis for the quantitative portions of this report. A full
analysis of the responses from the normal animals is beyond the scope
of this paper and will be considered elsewhere. The experiments
conformed to the Guide for the Care and Use of Laboratory Animals
(National Research Council 1996
) and were approved by the Institutional Animal Care and Use Committee.
Surgical procedures have been described in detail before
(Yakushin et al. 1995
, 1998
). Briefly, using sterile
surgical techniques, head bolts were implanted on the skull in dental
acrylic cement under general anesthesia. This provided for painless
fixation of the head in stereotaxic coordinates during testing.
Movements of one eye were recorded with two implanted scleral search
coils. One coil, in the frontal plane, measured horizontal and vertical eye position (Judge et al. 1980
). A second coil, placed
approximately orthogonal to the frontal coil, measured roll eye
position (Cohen et al. 1992
; Dai et al.
1994
). The semicircular canals were plugged about 1 mo after
coil implantation. The bony and membranous canals were identified and
interrupted by grinding across them with a fine diamond burr
(Cohen et al. 1964
, 1965
; Money and Scott
1962
; Suzuki and Cohen 1966
; Suzuki et
al. 1964
, 1991
, 1995
; Yakushin et al. 1995
). The
orifice of the canals was packed with bone dust, and the animals were
allowed adequate time to recover.
At the end of testing, one of the two animals whose canals were plugged (M9308) was perfused through the heart with saline and a paraformaldehyde/formalin solution under deep anesthesia. The temporal bones were removed, decalcified, embedded in celloidin, and processed for anatomical study. On histological examination, the bone had fused to provide an impenetrable block to the flow of endolymph in all six semicircular canals. Examples from the left labyrinth are shown in Fig. 1, A-C. The lateral canal plugs were located in the middle of the limb of the canals. The anterior canal plugs were closer to the ampulla, and the posterior canal plugs were located in the tail close to the common crus of the canal. The approximate position of the plugs in one of the labyrinths is shown in Fig. 4A. The hair cells of the canals (Fig. 1, A-C), the otolith organs (Fig. 1, D and E), and the cochlea (Fig. 1F) were intact.
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During testing, the monkeys' heads were fixed in a frame that held two
sets of field coils. The axes of the field coils were along the
interaural and dorso-ventral axes of the head, establishing a
head-fixed reference frame for measuring the orientation of the search
coils in front and on top of the eye. Data were recorded with
amplifiers having a band-pass of DC to 40 Hz. A computer controlled the
equipment and acquired the data. Voltages were digitized at 600 Hz/channel with 12-bit resolution. Coil related voltages were converted
to Euler angles. Eye position voltages were smoothed and digitally
differentiated by finding the slope of the least-squares linear fit,
corresponding to a filter with a 3-dB cutoff above 40 Hz, the cutoff
frequency of the filters used for data acquisition. Saccades were
eliminated using maximum likelihood ratio criteria (Singh et al.
1981
).
Eye velocities were calibrated by rotating the animals in light at
30°/s about the pitch, roll, and yaw axis. It was assumed that
horizontal and vertical (VOR) gains were approximately one (Crawford and Vilis 1991
; Dai et al.
1991
; Raphan et al. 1979
; Robinson
1963
). Roll gains were assumed to be 0.6 when rotation was
around a naso-occipital axis aligned with the spatial vertical (Crawford and Vilis 1991
; Henn et al.
1992
; Yakushin et al. 1995
). Roll gains derived
using this assumption agreed with those determined for monkeys using
other techniques (Dai et al. 1994
; Telford et al.
1996
; Yue et al. 1994
). After canal plugging,
optokinetic nystagmus (OKN) and OKAN were unaltered and acceleration
gains for steps of velocity were close to those before plugging
(Yakushin et al. 1998
). Consequently, it was determined
that the eye movement calibrations were unaltered after plugging. Eye
velocities to the left, down, and clockwise from the animal's point of
view were positive according to a right-hand rule and are represented by upward deflections in the velocity traces in Figs.
2-4.
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During testing, animals sat in a primate chair in a multi-axis
vestibular stimulator (Neurokinetics) that provided a light-tight environment and was used for calibration. To receive caloric
stimulation, the monkeys were positioned upright, right-side down
(RSD), left-side down (LSD), supine, and prone. When animals were
upright, the head yaw axis, which was normal to the horizontal
stereotaxic plane, was along the earth-vertical, and the lateral canals
were
30° above the horizontal stereotaxic plane (Blanks et
al. 1985
; Reisine et al. 1988
). In the supine
and prone positions, the lateral canals were tilted
30° from the
earth vertical plane, but the ampullae were oppositely directed
relative to the spatial vertical when face up or face down. The lateral
canals were aligned with the earth-vertical in the RSD and LSD
positions, the positions of maximal activation for convection currents,
assuming that the dihedral angle between the lateral canals was zero.
These head orientations were chosen because they have commonly been
used for studying the spatial orientation of velocity storage
(Dai et al. 1991
; Raphan and Sturm 1991
).
Time constants would be maximal for yaw when the animals were upright,
for pitch when the animals were side-down, and for roll when they were
supine or prone.
Caloric stimuli consisted of irrigation of one ear with 10 ml of cold
water at
20°C over 15 s. Before stimulation, a 22-gauge plastic tube, calibrated for length, was introduced into the external auditory canal. A shoulder attached to the plastic ensured that the
tube delivered water to within 1-3 mm from the drum, but did not
puncture it. The external canal was first irrigated with 200 ml of
37°C water to clean out cerumen. The drum was inspected before and
after irrigation to ensure that it had not been physically disturbed
and that there was no wax in the external canal. At the end of each
irrigation, the lights were extinguished, and the response was recorded
in total darkness. A 5-min interval in light was allowed to elapse
between stimuli to avoid residual cooling in the temporal bones. The
order of testing was upright, LSD, RSD, supine, and then prone, because
the caloric responses were approximately equal and did not appear to
habituate in this order in normal monkeys.
Computation of orientation vectors
It was assumed that caloric stimulation had altered activity in
the eighth nerve to excite velocity storage (Raphan and Cohen 1981
). We, therefore, utilized a method developed for computing the eigenvectors of velocity storage during OKAN and postrotatory nystagmus (Raphan and Sturm 1991
; Raphan et al.
1992a
) to compute the orientation vectors during caloric
stimulation. Briefly, the eigenvector of the three-dimensional eye
velocity response is the best fitting tangent line to the eye velocity
trajectory as it approaches zero in state space (Raphan and
Sturm 1991
; Raphan et al. 1992a
). At this time,
the activity in the vestibular nerve is presumably close or back to its
resting level, and the sole contribution to the response is from
velocity storage in the central vestibular system.
It was shown in early studies of visual suppression of per- and
postrotatory response (Raphan et al. 1979
) and OKN/OKAN
(Cohen et al. 1977
) that velocity storage is dumped with
a time constant of 1-2 s when monkeys view a subject-stationary visual
surround. If the lights are turned off, recovery of the nystagmus is
due to a mixture of activity from the canal nerve and the excitation of
velocity storage. When activity has ceased in the canal nerve, velocity
storage is no longer activated when the lights are extinguished after a
period of visual suppression. This was utilized to determine the
duration of action of caloric stimulation at the canals (Arai et
al. 2000
). Animals were subjected to increasing periods of visual suppression, and their ability to re-excite velocity storage was
assessed after the various periods of suppression. From this, it was
determined that there was no further re-excitation, and eye velocity
never recovered if the suppression duration exceeded 110 s, the time it
took for the normal response to decline to about 37% of the
culmination velocity. Therefore to estimate the eigenvector, the data
of the caloric response was windowed for left and right ear irrigation
after it declined to 37% of the peak value (Fig. 2, A and
B, double-headed arrows). The trajectory was fit by a
straight line in three-dimensional space using a minimum mean square
error criterion (Raphan and Sturm 1991
). The three-dimensional orientation was obtained from the vector along this
line (Fig. 2, A and B, 3 × 1 matrices). The
projections of the orientation vector in the yaw-roll, yaw-pitch, and
pitch-roll planes were obtained from the components of the vector in
the appropriate plane (Fig. 2C, left gray,
right black). To compare the orientation vectors for each
head position, the vectors were normalized from the 37% point.
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RESULTS |
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Data presented in this study were obtained 1-2 yr after canal
plugging so that the animals had fully recovered from the acute effects
of operation. Canal plugging was verified both physiologically and
anatomically in one of the animals (Fig. 1) and physiologically in the
other. After all six canals are plugged, there is a characteristic loss
of the vestibulo-ocular response to sinusoidal rotation at 0.2 Hz,
60°/s peak velocity. However, gains and phases normalize as the
animals are rotated at higher frequencies, due to the reduction in the
dominant time constant of the canals to 0.07 ms (Yakushin et al.
1998
).
Caloric responses of normal animals
In the upright position, cold caloric stimulation of the left ear
induced nystagmus with slow phase velocity to the left along the
positive z direction (Fig. 3B,
bottom). There were also clockwise (+x; Fig.
3B, top) and upward (
y; Fig.
3B, middle) components. Yaw (horizontal) slow
phase eye velocity rose to a peak value, culminating at approximately
175°/s about 30 s after the start of irrigation and then
declined monotonically to zero. The duration of the response was
approximately 120 s. Secondary caloric nystagmus then appeared,
but it will not be considered in this paper.
With the animal supine (Fig. 3C), the induced nystagmus had
a dominant yaw component to the animal's left (+z). There
was also a roll component, as when upright, but the pitch component was
reversed. In the prone position (Fig. 3D), the yaw component of the induced nystagmus was to the animal's right (
z),
the reverse of that when the animal was upright or supine. The pitch
and roll components were similar to those in the upright position, but were substantially larger. Since the x axis was aligned with
the spatial vertical in the prone position, these increases tended to
shift the orientation of eye velocity vector closer to the upward
spatial direction, although the increased yaw component limited this shift.
With the left side down (Fig. 3E), irrigation of the left
ear produced a strong leftward (+z) yaw component of eye
velocity with a clockwise torsional component. A strong upward
(
y) pitch component relative to the head was present in
this position. Since in this position, the pitch axis was aligned with
the spatial vertical, the eye velocity vector was again close to the
upward spatial vertical. The peak pitch component of the nystagmus
culminated about 20 s after the culmination of the yaw response
(Fig. 3E, middle).
When the animal was right side down (Fig. 3F), the yaw
component reversed and was to the right (
z), but the pitch
component remained upward, generating a spatially downward component.
There was negligible roll. Thus the vector of eye velocity was
spatially downward. Average peak values for the individual eye velocity components at the culmination of the nystagmus and the time course of
caloric nystagmus induced by stimulation of the left and right ears in
five normal animals, listed in Table 1,
were generally consistent with the responses shown in Fig. 3.
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Caloric responses of animals with all six canals plugged (NC animals)
Despite interruption of endolymph flow after plugging, robust
horizontal nystagmus was induced in all head orientations by caloric
stimuli (Fig. 4, B-F). Average values of the eye velocities at the points of culmination are given in Table 1. In contrast to the
responses before operation, the yaw eye velocity was always to the
ipsilateral side. After irrigation of the left ear, the spatial
direction of the eye velocity vector was predominantly along the head
vertical (+z) when upright and supine (Fig. 4, B
and C) but moved toward the spatial vertical when prone due to the counter-clockwise roll (
x) and leftward yaw
(+z) components (Fig. 4D). The velocity vector
also moved to the spatial vertical when LSD as a result of the leftward
yaw (+z) and upward pitch (
y) components (Fig.
4E). The roll component in the LSD position (Fig.
4E, top,
x) was not of sufficient
magnitude to alter the dominant direction of the eye velocity vector.
The eye velocity components were different when the animal was right
side down (Fig. 3F). As before, the yaw eye velocity was to
the left (+z), but the direction of the pitch component was
reversed (Fig. 4F, middle, down, +y),
producing an oppositely directed eye velocity vector.
Characteristics of the three-dimensional orientation in plugged animals
Since plugging the canals had eliminated convective endolymph
flow, the same activity was transmitted in the vestibular nerve to the
CNS after each caloric stimulus, regardless of head position in regard
to gravity. As a result, the spatial orientation of the caloric
response and the contribution of velocity storage to this orientation
could be studied in isolation. Therefore we first analyzed the spatial
orientation of the responses in the canal-plugged animals. In the
upright position (Fig.
5A), the average vectors for positive and negative yaw stimulation induced by
left (gray) and right (black) ear stimulation were close to the yaw
axis for both monkeys (+z, left ear stimulation;
z, right ear stimulation), and there was little roll (Fig.
5A1) or pitch (Fig. 5A2). In the supine position,
one monkey had a response along the head vertical, similar to the
upright condition, while another animal had a strong roll and a weaker
pitch component, which brought the average vector closer to the spatial
vertical [+x (gray) for left ear stimulation;
x (black) for right ear stimulation; Fig. 5, B1
and B2]. The average vector for the two animals had a yaw
component of about 77% of the total length of the vector (Fig.
5B3).
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When prone, the vectors in both monkeys were approximately the same,
having a significant roll component, which again brought the average
vector closer to the spatial vertical (
x for left ear
stimulation; +x for right ear stimulation; Fig.
5C3). This was opposite to the direction when the animals
were supine, since the spatial vertical had been inverted relative to
the head. The average contribution of the yaw component to the
orientation vector was reduced to about 38% of the total length of the
vector (Fig. 5C3), compared with 97% in the upright
position (Fig. 5C1), and the contribution of the roll
component was increased from about 15% to about 90% of the total
length of the vector (Fig. 5C3). The increase in the pitch
component from the upright to the supine-prone position was small
(about 5%). Thus the dominant orientation changes in both the supine
and prone positions were in roll, toward the spatial vertical.
Irrigation in side-down positions (Fig. 5, D and
E) had similar effects in aligning the nystagmus to the
spatial vertical. The relative contribution of yaw fell from about 97%
of the total length of the vector to 45%, and the contribution in
pitch increased from about 15 to 70% (Fig. 5, D2,
D3, E2, and E3). In the side-down positions, the roll component was not affected (Fig. 5, D1
and E1). In each instance, as for supine and prone, a pitch
component was induced along the spatial vertical in the same direction
as the yaw component in the head frame. Thus for left ear down, the pitch was negative (
y) for left ear irrigation and
positive (+y) for right ear irrigation. These vectors were
reversed when the right ear was down. The average roll components were
small in the side down positions. Thus the dominant effect of
unilateral caloric stimulation in all head positions was to induce
spatial components of slow phase eye velocity components whose
direction in space was the same as the direction of the yaw component
in the head coordinate frame.
Characteristics of the three-dimensional orientation in normal animals
In normal animals, convection currents toward or away from gravity
in the individual canals substantially enhanced or modified the
responses of the canal-plugged condition. In upright and supine positions, the yaw component of eye velocity was toward the irrigated ear as in the plugged animals (Fig. 6,
A and B). In addition, when the yaw component was
positive with the animal supine, the roll component was also positive,
as in the plugged condition and consistent with the organizational
scheme inherent in velocity storage (Dai et al. 1991
;
Raphan and Cohen 1988
; Raphan and Sturm 1991
; Raphan et al. 1992a
). In prone position,
the response was toward the contralateral ear (Fig. 6, C1
and C2), opposite to the canal-plugged response pattern
(note changes in the direction of yaw in Fig. 6, C1-C3).
This indicates that the convection currents were strong enough to
reverse any nerve-induced cooling response. In LSD position (Fig. 6,
D1-D3), convection currents induced eye velocities whose
vector was along the +z direction for both right and left
ear stimulation. Similarly, while in the RSD position, the yaw
component of the eye velocity was along the
z direction, regardless of the ear that had been stimulated (Fig. 6,
E1-E3). The generated +z component was
associated with a
y component for left ear down, and
z component was associated with a
y component for right ear down (Fig. 6, D3 and E3). Thus
regardless of head orientation during stimulation, the associated pitch
component was in the same spatial direction as the induced yaw
component relative to the head coordinate frame. The components of the
cross-coupled nystagmus had magnitudes, which rotated the orientation
vector consistent with the up-down asymmetries in time constant
observed for vertically induced vestibular nystagmus and OKAN
(Matsuo and Cohen 1984
; Raphan and Cohen
1988
).
|
Modeling canal activations as a function of head orientation
To gain insight into the component contributions to the caloric
response, the model of three-dimensional eye velocity generation developed by Yakushin et al. (1995
, 1998
) was utilized
to infer how activations related to specific canal planes would induce the observed eye velocities. These planes are consistent with the
planes determined anatomically and from physiological recordings (Blanks et al. 1985
; Reisine et al.
1988
). It was assumed that excitation of the canal nerves
corresponded to positive directions of activation of the canal planes,
which would be induced by equivalent positive direction of head
rotations. For the left labyrinth, the positive directions of movement
would be a head movement to the left for left lateral canal
stimulation, 45° down-left for left anterior canal stimulation, and
45° up-left for left posterior canal stimulation (Fig.
7A,
zC,
xC, and
yC). Compensatory eye rotations would
be opposite to these excitations, in accordance with the eye movements
produced by electrical stimulation of the ampullary nerves on the left
side (Cohen et al. 1964
; Suzuki et al.
1964
). We further assumed that cooling of the nerve would produce equal inhibition of the canal nerves on the left side, and that
this would be approximately 25-30% of the total response (Minor and Goldberg 1990
). Although the operations on
the temporal bone had eliminated the mastoid and other cavities that
existed before, conduction through the temporal bone was considered to be the major source of the cooling (Feldmann et al.
1991
). It was therefore assumed that the cooling equally
inhibited all canal nerves. The eye velocity orientation vector
was also chosen as 

0.3,
0.3,
0.3).
|
When this vector was inserted into the model, it generated an eye
velocity vector close to the roll (
x) direction, having components (
1, 0, 0.02) in head coordinates (Fig. 7A,
"Eye Velocity 1"). This eye velocity did not correspond to the
observed eye velocity vector (Fig. 7A, "Actual Eye
Velocity"), which had its dominant component along the z
axis (
0.09, 0.19, 0.98). There was no set of negative canal
activations that could generate an eye velocity vector outside the
sector defined by the canal vectors to predict the actual direction of
eye velocity. Therefore inhibition of the canal nerves alone could not
have produced the observed eye velocity.
To correct for this deficiency, the canal activations were modified on
the assumption that the cooling had caused contraction of the endolymph
between the plug and the cupula. This would cause deviation of the hair
cells in the direction of the plug in all three canals, similar to the
utriculofugal (ampullofugal) deflections produced in normals by
convection. Ampullofugal flow of endolymph produces inhibition of the
lateral canal nerves (
zC) and
excitation of the anterior (+xC) and
posterior (+yC) canal nerves, as shown by the curved arrows in Fig. 4A (Ewald 1892
).
Therefore we modified the canal activation vectors to increase the
inhibition of the lateral canal afferent activity and to generate
excitation of the anterior and posterior canal nerves. We assumed that
the equal inhibition of the canal nerves added to the inhibition and
excitation produced by this ampullofugal deflection. Consequently, the
vector was chosen as 0.5, 0.5,
0.75. This produced a resultant eye
velocity direction that closely approximated the eye velocity vector in the canal-plugged animal when upright (Fig. 7B, "Eye
Velocity 2").
It should be noted that the explicit values used to model the data are not unique. The critical constraint is that the anterior and posterior canal activation values should be the same and positive, and the lateral canal activation should be negative. The reverse, inhibition of the anterior and posterior canal nerves and excitation of the lateral canal nerve, would have produced an eye velocity in the opposite direction and could not have fit the data. The approximation of the observed response, while close to the "Actual Eye Velocity" in the upright position, may have arisen due to lateral canal inhibition alone, with no contribution from the vertical canals, and velocity storage, which is oriented toward the spatial vertical, could then have provided additional rotation toward the spatial vertical. However, this would still have required the proposed contraction mechanism, which countered the inhibition due to cooling of the nerves of the vertical canals, effectively zeroing their responses, while increasing the inhibition of the lateral canal nerve.
We tested the hypothesis that velocity storage contributed to the orientation of the caloric response by considering the model predictions for tilted head positions. Because the nature of the cooling was the same in every head orientation, it would be expected that eye velocity would be the same in all positions (Fig. 7, C-F, "Eye Velocity 2"), if no other factors were involved. This did not occur. For example, the "Actual Eye Velocity" vectors were significantly different from the direction of "Eye Velocity 2" for side down (LSD and RSD), supine, and prone positions (Fig. 7, C-F). In LSD and RSD, the actual eye velocity vector had a large pitch component, while in supine and prone, and there was a large roll component that shifted the eye velocity vector toward the spatial vertical. Because of the absence of convection currents in the canal-plugged animals, the most likely cause for this substantial shift in the direction of the eye velocity vector is the spatial orientation of velocity storage. Velocity storage also probably contributed to orienting the eye velocity in the upright position toward the spatial vertical.
Because of the substantial contributions of convection currents in the normal animal, and the lack of understanding of how convection currents might be induced in all canals in the various head positions, it was premature to speculate on the basis of the evidence presented here how to model the normal response.
| |
DISCUSSION |
|---|
|
|
|---|
This study shows that caloric nystagmus is readily induced in
monkeys after plugging all six canals had eliminated endolymph flow due
to convection. Primary evidence for the absence of convective flow
comes from the demonstration that the canals were occluded by bone,
leaving only a small space between the plug and the ampulla. This
precluded fluid flow that would significantly deflect the cupula and
activate the nerve. Supporting this, we have previously shown in these
same animals that this occlusion reduced the time constant of the
canals by almost two orders of magnitude (Yakushin et al. 1995
,
1998
). As a result, the gain of the angular vestibulo-ocular reflex (aVOR) fell to zero at low frequency head rotations (0.2 Hz;
Yakushin et al. 1995
, 1998
), requiring high frequencies
of acceleration to induce enough flow to produce significant eye velocity (Lasker et al. 1999
; Rabbitt et al.
1999
, 2001
; Yakushin et al. 1998
). These
frequencies are well out of the range of the frequency content of any
convection current that might be produced by the caloric stimulus.
Other evidence for the lack of convective flow after plugging comes
from a comparison of the horizontal component of the nystagmus in the
normal and canal-plugged animals. The slow phase velocity of the yaw
component in the normal animal varied according to head position in
regard to gravity. The velocities were always toward the left
(+z) when either ear was stimulated in the LSD positions and
to the right (
z) in the RSD positions (Fig. 3, E and F, and Fig. 6, D and
E). Similarly, the yaw component of the response was
reversed in the normal animal in the prone and supine positions (Fig.
3, C and D, and Fig. 6, B and
C). Left ear stimulation produced eye velocity to the left
when supine and to the right when prone. These direction changes were
presumably due to changes in direction of convection flow in the
lateral canal. In contrast, the yaw component of eye velocity in the
plugged canal animals was always toward the ipsilateral ear regardless of head orientation (Fig. 4). Similar results have been reported after
lateral canal plugging by Paige (1985)
.
With convection flow eliminated, the following question arises: what
other factors were responsible for the caloric responses in the
canal-plugged animals? There is evidence that thermal effects on the
nerve play a role in generating the caloric response (Coats and
Smith 1967
; Minor and Goldberg 1990
;
Paige 1985
). Minor and Goldberg (1990)
,
using a model of Paige (1985)
, concluded that nerve
cooling contributes about 30% of the eye movement response. In our
model of the caloric response in canal-plugged animals, we first
assumed that cooling of the vestibular nerve reduced the firing rates
about 30% equally in all branches of the vestibular nerve (Fig.
7A, "Eye Velocity 1"). It was not possible, however, using only nerve cooling to predict the caloric eye velocity responses in the canal-plugged animal in any of the head positions. The reason
for this was that equivalent inhibition of the activity from each canal
would produce a predominant response along the roll direction, or about
90° from the observed response in the upright condition.
Even if the change in the bone temperature were not distributed
uniformly, the cooling would still induce inhibition of the canal nerve
activity in all canals. This would maintain the eye velocity vector
within the solid angle defined by the normals to the canal planes. The
experimentally observed eye velocity orientation vector moved outside
this solid angle. Since velocity storage does not orient from roll to
yaw, but only from yaw to roll (Dai et al. 1992
;
Raphan and Cohen 1996
; Raphan and Sturm 1991
; Raphan et al. 1992a
; Wearne et al.
1999
), reverse cross-coupling could not have contributed to the
observed orientation of eye velocity which was predominantly along the
yaw axis. Therefore the direction of eye velocity in the upright
condition could not be explained by nerve cooling alone, and other
factors must be present to account for the caloric response after canal plugging.
Based on their experiments on caloric nystagmus in microgravity,
Scherer and Clarke (1985)
proposed that unequal fluid
contraction on the two sides of the cupula in the lateral canals was
largely responsible for the caloric nystagmus that was observed in
space in the absence of convection currents. Minor and Goldberg
(1990)
concluded that thermal expansion of the endolymph fluid
would not contribute significantly to the caloric response in normal subjects because induced pressure effects would be rapidly normalized to both sides of the cupula. Furthermore, they argued that there would
be no sustained activation of canal afferents and the activity would
decay with the cupula-endolymph time constant of 5 s. This controversy is still unsettled, but fluid contraction could play a
significant role in generating the three-dimensional eye velocity response in the canal plugged animals due to differential pressure on
the cupula created by contraction of different column lengths on either
side of the plug. Scherer and Clarke (1985)
estimated the pressure differential across the cupula (P) at about
10
2 dynes/cm2, which is
an order of magnitude beyond the threshold for activating the hair
cells innervating the canal ampulla (Oman and Young
1969
; Steer et al. 1968
). The net effect of this
deflection would be to mimic utriculofugal (ampullofugal) endolymph
flow resulting from cooling that produced convection currents, thereby
producing inhibition in the lateral canal and excitation in the
anterior and posterior canals.
We reasoned that it was likely that contraction of endolymph between the cupula and the plug had occurred in our experiments because the plugging did not allow fluid to circulate freely and therefore gave a more sustained response than in normal canals. With the introduction of the predicted excitation of the anterior and posterior canals and inhibition of the lateral canals, the model almost exactly predicted the eye velocity that was observed in the upright condition (Fig. 7, "Eye Velocity 2"). We would emphasize that although the exact weights for canal activations were unknown in our simulations, the constraint that the anterior and posterior activations must be equal or close to each other, imposes a structure on the signs of the canal activations that we have postulated. This strongly suggests that a pressure differential across the cupula may have been present in the canal-plugged animals to contribute to the observed response. The finding that horizontal caloric nystagmus could not have been produced simply by inhibition and excitation due to equivalent cooling or heating of the canal nerves on one side in our monkeys, supports the conclusion of Scherer and Clarke that a pressure differential across the cupula may have been operative to produce horizontal (+z axis) caloric nystagmus in microgravity.
Addition of these two components did not predict the orientation of eye
velocity in side down, prone and supine positions in the canal plugged
animals, however, and the eye velocity of the caloric nystagmus was not
maintained along the z axis, as when the animals were in the
upright position. Rather, the predicted eye velocities would have
remained along the head z axis and would have pointed along
the spatial horizontal in the side down and prone/supine positions.
Instead, the cross-coupled pitch components in side-down positions and
roll components in supine/prone positions tended to align the eye
velocity vector with the spatial vertical, respectively. Moreover, the
velocity vectors were directed along the spatial vertical with the same
polarity as the yaw velocity in the head frame. Thus if yaw eye
velocity was to the left (+z), then the pitch and roll
components for side-down and prone/supine positions were along the
positive direction in space. These were (+x) for supine,
(
x) for prone, (
y) for LSD, and
(+y) for RSD positions. The reverse would be true if yaw eye
velocity was to the right (
z). These orientations of the
velocity vectors to the spatial vertical are similar to the
orientations of OKN/OKAN and postrotatory nystagmus in tilted positions
(Dai et al. 1991
, 1992
; Raphan and Sturm
1991
; Raphan et al. 1992a
). We have previously shown that the orientation properties of velocity storage are unaltered
after canal plugging (Raphan et al. 1992b
).
Therefore we conclude that velocity storage and its inherent
orientation properties play a significant role in orienting the
velocity vector of caloric nystagmus toward the spatial vertical.
Although the trajectories of the caloric response were curved in
velocity space, it should be understood that they represent the dynamic
responses of a system that includes a number of responses in its early
portions. The actual orientation vectors, i.e., the eigenvectors of the
velocity storage system, are fixed in the head and can be estimated
only from the data over the time period during which eye velocity was
<37% of the culmination or when cupular activation had presumably
declined to zero. Although velocity storage is likely to play a
significant role in orienting eye velocity toward the spatial vertical
in tilted positions of the head, previous work has demonstrated that
velocity storage only orients responses from yaw to other directions
and not from roll or pitch to yaw (Dai et al. 1991
,
1992
; Raphan and Sturm 1991
; Raphan et
al. 1992a
; Wearne et al. 1999
). Since the
response from nerve cooling was along the roll direction, there could
have been no cross-coupling from roll to yaw, and this possibility was
rejected. Thus velocity storage stands as an independent mechanism for
orienting caloric responses, separate from the contraction due to
cooling of the endolymph. While velocity storage is weaker in humans
than in monkeys, the relative cross-coupling is sufficient to orient eye velocity toward the acceleration of gravity, as in the monkey (Gizzi et al. 1994
). Thus the three-dimensional caloric
responses in humans may be directly extrapolated from the responses in
the monkey.
The evidence presented in this paper cannot be used to explain the
normal caloric response, because there is insufficient information
about whether and how convection currents are induced in the three
canals in the various head positions. There is data on this (Aw
et al. 1998
, 2000
; Böhmer et al. 1992
, 1995
,
1996
; Fetter et al. 1998
), but it is inadequate
to make quantitative predictions as to the nature of this activity.
Some global observations can be made, however. The induced eye
velocities produced by cold caloric stimulation of the normal animal
were consistent in each position with the convective flow of endolymph
in the lateral canals toward gravity, which appears to be a dominant
factor in producing the various responses (Fig. 6). Thus in the upright and supine positions, cold irrigation produced yaw eye velocity to the
left (+z) for left ear irrigation and to the right
(
z) for right ear irrigation, consistent with ampullofugal
convective flow in the lateral canal on the irrigated side. These
directions were reversed in the prone position, consistent with an
ampullopetal flow. Left ear down produced leftward eye velocity for
both left ear and right ear irrigation, consistent with ampullopetal
flow in the left lateral canal and ampullofugal flow in the right
lateral canal. Right ear down produced the opposite effect generating rightward eye velocity (
z) for both right ear and left ear
irrigation. The downward, counterclockwise components in the upright
position most likely originated from ampullopetal flow in the anterior canal, which caused inhibition of anterior canal activity. The downward
and clockwise components in the supine position probably originated
from ampullofugal flow in the anterior and posterior canals. Reversal
of these currents in the prone position would produce the upward component.
As in the canal-plugged condition, the orientation of the eye velocity was also consistent with the orientation properties of velocity storage. This produced a positive roll component (+x) for positive yaw eye velocity, induced when the animal was supine, and a negative roll component when negative yaw eye velocity was induced. When the induced yaw eye velocity was reversed for prone position, the direction of the induced roll component was maintained the same in head coordinates since the positive roll direction was reversed in space (+x is pointing down in space). Right ear and left ear down produced corresponding spatial pitch components consistent with the direction of the induced yaw component in head coordinates. Thus velocity storage is likely to play an important role in orienting the caloric response in normal animals as well as in monkeys with plugged canals.
In summary, we have considered four dominant mechanisms that could have contributed to caloric responses in the normal animal: convections currents, nerve cooling, pressure gradients across the cupula due to endolymph contractions as a result of cooling, and velocity storage. Canal plugging, which eliminated convection, was useful in demonstrating that contraction of the endolymph by cold, and presumably expansion by hot, stimulation can also contribute to the caloric response. In addition, the role of the orientation properties of velocity storage were particularly evident after canal plugging and are likely to play an important role in the orienting the caloric responses in normal animals.
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ACKNOWLEDGMENTS |
|---|
We thank Dr. Mingjia Dai for assistance in obtaining data, Dr. Mikhail Kunin for writing the programs for model prediction of the data, and V. Rodriguez for technical assistance.
This study was supported by the Japanese National Science and Research Fund 11671707 and by National Institute of Health Grants DC-03787, DC-03284, DC-04996, EY-11812, EY-04148, and EY-01867.
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FOOTNOTES |
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Address for reprint requests: T. Raphan, Dept. of Computer and Information Science, Brooklyn College of the City University of New York, 2900 Bedford Ave., Brooklyn, NY, 11210 (E-mail: raphan{at}nsi.brooklyn.cuny.edu).
Received 7 January 2002; accepted in final form 12 April 2002.
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REFERENCES |
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