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. Author manuscript; available in PMC: 2026 Mar 10.
Published in final edited form as: Adv Space Biol Med. 2005;10:105–164. doi: 10.1016/s1569-2574(05)10005-7

Vestibular Experiments in Space

Bernard Cohen 1, Sergei B Yakushin 1, Gay R Holstein 1, Mingjia Dai 1, David L Tomko 2, Anatole M Badakva 3, Inessa B Kozlovskaya 3
PMCID: PMC12969068  NIHMSID: NIHMS2145269  PMID: 16101106

Introduction

Life on Earth is conditioned by the constant downward pull of gravity, which can be considered as an equivalent constant upward linear acceleration (Einstein, 1911). During lateral, fore-aft, and vertical translations as well as during centripetal accelerations generated by turning around distant axes, these linear accelerations summate with the linear acceleration of gravity to form a resultant vector, which we term gravito-inertial acceleration (GIA). These linear accelerations increase the magnitude of the GIA and tilt it relative to the head. The otolith organs and body tilt receptors sense the resultant changes in the GIA and generate compensatory and orienting eye movements through the linear vestibulo-ocular reflex (lVOR) to direct and stabilize vision. Angular head movements are sensed by the semicircular canals, which produce compensatory eye movements over the angular vestibulo-ocular reflex (aVOR). The vestibular system also responds to linear and angular accelerations through vestibulo-spinal reflexes to produce body postural movements that stabilize the body when stationary and support it when one is in motion. Additionally, the vestibular system responds to changes in head and body position relative to the GIA to maintain blood pressure and enhance respiration. Thus, the vestibular system plays a critical role in sensing and responding to linear and angular accelerations in a gravitational environment.

In microgravity, the linear acceleration of gravity is reduced to negligible levels, and a standing posture is no longer maintained. Instead, subjects swim in Space rather than walk, and they no longer experience the vertical linear translations that accompany locomotion. Additionally, gravity no longer contributes to the resultant change in the GIA when the head is translated. Thus, the GIA is always in the direction of the translational and centripetal accelerations due to movement. Angular acceleration, which is in a head coordinate frame, is not markedly altered in microgravity. Because of the ubiquitous nature of gravity on Earth and the difficulty of performing experiments on orbit, we know relatively little about how the nervous system is altered by the prolonged absence of gravity.

From the 1970s, the Russian Space Agency made orbital space flight available to INTERCOSMOS scientists from many countries for animal experimentation, primarily on rats. This included Czechoslovakia, Poland, Hungary, Germany, France, and the United States. Between 1983 and 1995, monkeys and rats flew for approximately 1–2 week periods on a Vostok Space Capsule in experiments supported by the Russian Space Agency and the National Aeronautics and Space Aadministration (NASA). Rodents and invertebrates also flew on NASA Space Shuttle missions, particularly on the Neurolab Mission (STS-90) in 1998. The purpose of this chapter is to provide a summary of these experiments. Experiments on rodents and other animal species in the NASA Space Shuttle flights and the Russian COSMOS/BION flights are summarized in the first section. The second section summarizes inflight experiments performed by the Russian Space Agency on the aVOR and on single unit activity in the vestibular nuclei and flocculus of monkeys. Many of these data appear here for the first time. In the third section, we summarize NASA-supported research on rhesus monkeys on the linear and angular vestibuloocular reflex (lVOR and aVOR). The intent was to provide a summary of experimental data on which future experimentation in Space can be expanded. In addition to revealing some new and interesting scientific results, it is hoped that it will become obvious that basic studies, involving subhuman primates as well as rodents should be essential components of any future space-related research. The results of the earliest flights are not included in this chapter, but can be found in references at the end of the bibliography.

SECTION 1: CELLULAR RESPONSES TO ALTERED GRAVITATIONAL ENVIRONMENTS IN ADULT ANIMALS

A number of studies have examined the impact of altered gravity exposure on vestibular system structures at the cellular level. As a whole, they clearly document the modifiability of cellular and subcellular constituents of vestibular pathways in response to altered gravitational stimuli.

Peripheral vestibular system

Some evidence suggests that exposure of adult as well as developing animals to altered gravitational environments can trigger adaptive responses in weight-lending structures. For example, an increase in otoconial mass has been reported in the utricles of adult animals of several species (rats, frogs) following 7 days of exposure to microgravity (Vinnikov et al., 1980; Ross et al., 1985; Ross, 1987; Lychakov et al., 1989). Conversely, the saccular otolithic membrane volume is reduced in rats exposed to 2.3 g or 4.15 g hypergravity through centrifugation (Lim et al., 1974), although otoconial morphology (examined by scanning electron microscopy) and otoconial synthesis (assessed by mRNA expression of the otoconial matrix protein osteopontin) appear to be normal after 2 h to 7 days of hypergravity exposure (Uno et al., 2000).

Increases in otoconial mass have also been observed in the saccular otoliths of newt larvae (Weiderhold et al., 1997) and late-stage embryos of swordtail fish (Weiderhold et al., 2000) reared in Space, although such increases are not observed in older fish. As in adult animals, the saccular otolithic membrane volume is reduced in cichlid fish reared on a centrifuge (Anken et al., 1998), and the volume of statoconia in marine mollusk larvae reared at 2–5 g is diminished in a graded manner as compared with 1 g controls (Pedrozo and Wiederhold, 1994). Similarly, there is a reduction in the number of large otoconia that are present in the anterior peripheral portion of the utricle in rats raised in a 2 g environment for 60 days than in 1 g controls (Krasnov, 1991). Taken together, these results suggest that otoconial mass adapts to fluctuations in the gravitational stimulus, perhaps to maintain a consistent force on the maculae.

A number of studies have addressed the question of morphologic alterations in the sensory hair cells of adult mammalian otolith organs in response to altered gravitational conditions. These studies indicate that short-term (e.g., 7 day) exposure to space flight does not cause otolith receptor cell degeneration in rats (Ross et al., 1985), although the type I hair cells reportedly exhibit abnormal cytologic features such as increased chromatin, and enlarged perinuclear and intercellular spaces (Krasnov, 1987, 1991). However, more prolonged exposure to microgravity clearly impacts hair cell synaptology. In general, these studies indicate that type II hair cells in particular, but also type I cells evidence adaptive structural modifications in response to alterations in the gravitational environment (Ross, 1993, 1994, 2000). Quantitative ultrastructural analysis of utricular hair cells from adult rats sacrificed immediately after landing from a 9-day space flight demonstrated statistically significant increases in the number of ribbon synapses (Ross, 1994). In addition, the number of synapse pairs and clusters markedly increased in the type II hair cells. Nine days after landing, which was the mission duration, synapse counts remained elevated in the flight rats, but were also elevated in the type II hair cells of ground control animals, suggesting that these receptor cells are particularly vulnerable to stress-induced morphologic changes. In a subsequent study (Ross and Tomko, 1998), the mean number of synapses on type II hair cells doubled, and those on type I cells increased by over 40% by the 13th day of a 14-day space flight. Immediately postflight, these synapse counts were reduced to 67% and 13% increases, respectively, over control values. Comparable studies of vestibular hair cells have been conducted utilizing 2–4 g hypergravity exposure for periods of time ranging from 14–30 days (Lim et al., 1974; Lychakov et al., 1988; Ross, 1993). In general, these experiments support Ross’ centrifugation study (Ross, 1993) demonstrating that type I hair cell synapse number does not change in response to hypergravity, but there is a decrement of approximately 40% in type II hair cell synapses. Clearly, the otolith organs of adult mammals have the potential for morphologic reorganization at several sites in response to altered gravity conditions (Ross, 1997).

Since studies of molecular changes in peripheral vestibular cells in response to fluctuations in the gravity stimulus have been initiated relatively recently, generalizations about molecular alterations are premature. One recent study investigated glutamate receptor mRNA expression using RT-PCR on cells of the vestibular ganglion, as well as the vestibular nuclei, and vestibulocerebellum of rats exposed to hypergravity for 2 h–7 days (Uno et al., 2002). In the vestibular periphery, this experiment demonstrated that synthesis of GluR2 (an AMPA glutamate receptor subunit) receptors in vestibular ganglion cells is reduced in rats exposed to 7 days of hypergravity.

Behavioral, physiological and biochemical correlates of vestibular cellular responses

A spinning movement during swimming, termed “looping,” was initially reported in some (but not all) fish at the transition from 1 g to microgravity during parabolic flight (von Baumgarten et al., 1972), and subsequently described in larval cichlid fish and Xenopus laevis immediately following prolonged 3 g centrifugation (Rahmann et al., 1992). Looping has also been reported in killifish in microgravity (von Baumgarten et al., 1975). Fish that evidence looping behavior exhibit a significantly higher asymmetry in otolith size (Anken et al., 1998) and weight (Beier et al., 2002), in comparison with nonlooping siblings. In addition, although the total number of sensory and supporting cells in the utricular maculae is the same, the cell density is significantly lower in looping than nonlooping fish, due to the atypical presence of enlarged epithelial cells (Bauerle et al., 2004).

Adult mammals may be more profoundly affected by changes in the gravitational environment than are fish. Upon landing following 9 days of space flight, adult rats reportedly show substantially reduced locomotion (Ross, 1994). They maintain a posture with their abdomens and tails flat against the cage floor, with their limbs and digits extended. After 9 days at 1 g, flight rats display normal body posture and movement. Similarly, after 14 days of exposure to 2 g through centrifugation, adult rats show profound deficits in righting responses, swimming and balance (Fox et al., 1992). Recovery of normal orientation during swimming requires 4–24 h at 1 g, whereas the righting reflex does not return to normal for 5–7 days (Ross and Tomko, 1998).

Neurophysiological studies have further documented an immediate post-flight alteration in vestibular activity (Boyle et al., 2001). Within the first 16 h post-space flight, utricular afferents in the oyster toadfish were hypersensitive to translational acceleration, but had no change in directional selectivity. The afferent sensitivity returned to baseline levels by approximately 30 h postflight. Since anamniotes such as the toadfish have only type II hair cells, the reported increase in ribbon synapse number (Ross, 1997) could be one explanation for the afferent hypersensitivity.

Central vestibular system

Several studies have addressed the impact of altered gravitational environments on cells of the central vestibular system. Most of these studies have examined the vestibular nuclei and/or vestibulo-cerebellum, and have utilized either a morphological approach, or a marker for cellular activity. Early studies of the cerebellar nodulus of adult rats exposed to 18 days of space flight revealed ultrastructural alterations in Purkinje cell dendrites and mossy fiber terminals (Krasnov and Dyachkova, 1986, 1990). In these studies, the major modification described in the Purkinje cells was a widening of the synaptic cleft at contacts with Purkinje cell dendrites. In mossy fiber terminals, structural alterations included densely packed synaptic vesicles, with unusual clustering of such vesicles near the presynaptic membranes of axodendritic synapses, increased electron density of pre- and postsynaptic membranes, and enlargement of the synaptic gap. Similar changes are observed in nodular mossy fiber terminals from rats flown on 5–7 day missions and sacrificed within 8 h of landing. Moreover, ultrastructural alterations in the primary somatosensory cortex of these flight animals included a profound decrement in the number of axodendritic synapses, and an increase in the number of axon terminals showing “light” degeneration, as well as signs of “superexcitation” including an increase in the number of axon terminals showing dark degeneration. In concert with this finding, increased numbers of synaptic contacts have been demonstrated in neonatal swordtail fish after 16 days in microgravity, specifically in the nucleus magnocellularis of the primary vestibular brainstem region, area octavolateralis (Ibsch et al., 2000).

More recently, the ultrastructure of the otolith-recipient zones of the cerebellar nodulus has been analyzed in tissue from flight and cage-control rats sacrificed in microgravity after 24 h of space flight (Holstein et al., 1999). Qualitative observations of this tissue indicate that several structural alterations occur in the neuropil, and in the Purkinje cell cytoplasm, of the nodulus of rats exposed to 24 h of space flight. These anatomical alterations are not apparent in the cage control animals. Most notably, the cisterns of smooth endoplasmic reticulum that are normally present throughout Purkinje cells are substantially enlarged and more complex in Purkinje cells of the otolith-recipient zones of the nodulus. The increased complexity of the cisterns results in the formation of long, stacked lamellar bodies that are observed throughout entire Purkinje cells, including the somata, dendrites, thorns, and axon terminals. In addition, occasional enormous mitochondria, >1 μm in cross-sectional diameter, are present in the Purkinje cell somata of flight animals. Ultrastructural indications of degeneration and synaptic reorganization are also observed in the molecular layer of the nodulus from the flight animals, but not cage controls. Since these morphologic changes are not apparent in control animals, they are not likely to be due to caging or tissue processing effects. The particular nature of the structural alterations, including the formation of lamellar bodies and the presence of degeneration, suggests that excitotoxity may play a role in the short-term neural response to space flight.

In the granular layer of the nodulus of rats raised in a 2 g environment for 60 days, 80% of the glomeruli showed altered synaptic morphology, including changes in the density of pre- and postsynaptic membranes, increased thickness of the postsynaptic density, enlargement of the synaptic cleft, increased packing density of synaptic vesicles, enlarged mitochondria, and an increase in the number of microtubules (Krasnov and Dyachkova, 1986; Krasnov, 1991). Two days after return to a 1 g environment, the ultrastructure of the nodulus resembles that of control animals. The synaptic vesicle packing density is decreased, and the number of microtubules is diminished, suggesting reversibility of the gravity-induced effects. Taken together with the microgravity findings, these results more generally indicate that the central vestibular system responds to major changes in the gravitational stimulus with similar morphological restructuring, regardless of the direction (hypo- or hyper-) of that change.

In light of the ultrastructural findings suggesting that excitotoxicity may be a factor in early neuronal responses to altered gravitational environments (Holstein et al., 1999), the recent study of glutamate receptor expression is of particular interest. This study examined glutamate receptor mRNA expression using RT-PCR on cells in the vestibular nuclei and vestibulo-cerebellum of rats exposed to hypergravity for 2 h to 7 days (Uno et al., 2002). The results indicate that mRNA expression of GluR2 (an AMPA glutamate receptor subunit) and NR1 (the obligatory subunit of the NMDA glutamate receptor) in the nodulus/uvula and NR1 expression in the medial vestibular nucleus increase after 2 h of stimulation. This expression gradually returns to baseline during the 7 days of hypergravity exposure. As noted above, mRNA expression of GluR2 receptors in vestibular ganglion cells is reduced after 7 days of stimulation. Neither the mGluR1 metabotropic receptor nor the δ2 glutamate receptor in the flocculus and nodulus/uvula is affected by hypergravity exposure for 2 h to 7 days. It was suggested that the immediate (2 h) adaptation to hypergravity involves enhanced cerebellar inhibition of the vestibular nuclei mediated by Purkinje cell NR1 and GluR2 receptors, whereas longer term adaptation involves decreased transmission from vestibular hair cells to primary afferent neurites mediated by down-regulation of postsynaptic GluR2 receptors on the primary afferents. One interesting aspect of this study is that functional NMDA receptors are not normally present on cerebellar Purkinje cells in adult mammals. Conceivably, an altered gravitational environment presents a sufficient stimulus to trigger their expression and activity. However, the activity of enzymes involved in energy metabolism (lactate dehydrogenase and creatinine kinase) in giant Deiters’ neurons of the lateral vestibular nucleus and cells of the cerebellar nodulus in rats are not appreciably affected by 22 days of space flight (Krasnov, 1975).

Space flight-related studies utilizing markers for vestibular neuronal activity have concentrated primarily on the immediate early gene c-fos. The gene encodes for Fos protein, which reaches peak values within 2–4 h of the effective stimulus and returns to baseline within 6–8 h. Fos-related antigen (FRA) proteins, which are generated by multiple genes, are induced shortly after stimulation, but persist for days (“acute” FRAs such as FRA-1, −2, FosB, ΔFosB) or weeks (“chronic” FRAs, e.g., modified forms of ΔFosB). Fos protein is often utilized as a neural activity marker, since it can be identified with higher spatial resolution than metabolic indicators. Although the basal expression level of c-fos expression is low in the brain, increases in Fos-like immunoreactivity have been reported in vestibular structures following galvanic stimulation (Kaufman and Perachio, 1994; Mashburn et al., 1997) and centripetal acceleration (Kaufman et al., 1992), as well as space flight.

Results from space flight experiments on adult rat brain tissue indicate a trend toward increased numbers of Fos-immunopositive cells in the vestibular brainstem (particularly the medial and descending vestibular nuclei, MVN and DVN, respectively) 24 h postlaunch, and a statistically significant increase in the number of immunostained cells 24 h after return from a 17-day mission (Pompeiano et al., 2002). The number of Fos-immunostained vestibular cells were equivalent in flight animals and ground controls by 13 days postlaunch and at 13 days postlanding. The pattern of FRA protein immunolabeling was qualitatively similar to that of Fos, except at 1 day after landing, when FRA-immunolabeled cells were observed throughout the entire DVN, but only in the caudal MVN while Fos staining was reported throughout the entire MVN. In addition, Fos- and FRA-like immunoreactivity in the vestibular portions of the inferior olivary complex of rats was unchanged 24 h postlaunch (d’Ascanio et al., 2003). However, while Fos immunolabeling remained unchanged 24 h postlanding in these regions of the inferior olive, increased FRA-immunostaining was reported at that time. The authors attribute these findings to the mixed sensory signals derived from rapid fluctuations in g-force during launch. In contrast, the flight rats sacrificed in microgravity 1 or 13 days postlaunch had fewer Fos- and FRA-immunolabeled efferent vestibular neurons than ground controls (Balaban et al., 2002), although no differences were observed between flight and control rats during the postlanding re-adaptation period. The results are interpreted as indicative of general physiological and morphological changes in the cells. Interestingly, Fos- and FRA-like immunoreactivity in autonomic regions such as area postrema and nucleus tractus solitarius of these flight rats were equivalent to control tissue during exposure to microgravity, but were significantly increased 24 h after landing (Pompeiano et al., 2004).

Upregulation of genomic activity has also been demonstrated in several brainstem nuclei related to otolith pathways, particularly the dorsomedial cell column of the inferior olivary complex as well as MVN, DVN and the y-group, in head-fixed rodents exposed to 2 g centripetal acceleration (Kaufman et al., 1992). This upregulation occurs following one-axis stimulation restricted to the plane of the saccule (Mashburn et al., 1997) or the utricle (Kaufman et al., 1991). Immunohistochemistry for fos protein and for FRA proteins has also been performed on vestibular tissue from 60-day-old rats exposed to 2 g or 4 g centrifugation in the plane of the saccule (hypergravity exposure), and in 60-day-old rats born and housed at 2 g, then exposed for 90 min to 1 g (hypogravity condition) (Duflo et al., 2000). This study found enhanced Fos-related labeling of the vestibular brainstem, particularly MVN, DVN, nucleus of Roller, the y-group and the inferior olivary nucleus, only in the hypergravity condition. Although the β subnucleus of the inferior olive was not immunostained in this study, nor in Mashburn et al.’s study (1997), it did display Fos-like immunoreactivity in the experiments of Kaufman and colleagues (Kaufman et al., 1992, 1993), suggesting that utricular rather than saccular inputs activate β-subnucleus Fos expression.

Summary

It is clear that cellular and subcellular constituents of the vestibular pathways are modified in response to altered gravitational stimuli. In the vestibular periphery, opposite structural effects appear to result from hypo- and hypergravity stimulation. In the central vestibular system, neural circuits may well exhibit apparently identical structural changes in response to diverse hypo- and hyper-gravity stimuli, reflecting the more dynamic, highly regulated interactions of the central pathways. More research will be needed to resolve the inconsistencies in the current published literature.

SECTION 2: STUDIES OF THE EFFECTS OF MICROGRAVITY ON VESTIBULAR AND OCULOMOTOR FUNCTION IN THE RUSSIAN COSMOS PROJECT

Abstract

Experiments were performed while monkeys flew in space in the “Cosmos/Bion” Missions to determine the effect of microgravity on the oculomotor and vestibular systems. Eye-head coordination during gaze shifts to lateral targets (gaze fixation reaction, GFR) and multiunit activity in the medial vestibular nuclei (MVN) and cerebellar flocculus were studied in rhesus monkeys in the Bion 6 (Cosmos 1514) through Bion 11 projects. In the first few days of space flight, gaze displacement onto lateral targets became hypermetric, and the amplitude of head movements decreased. This was compensated for by increases in the gain of the angular vestibulo-ocular reflex (aVOR) that could last for the duration of the missions. Associated with this, there were increases in neuronal activity in MVN and flocculus. Sensitivities of the same populations of MVN neurons to linear acceleration, in general, increased gradually over the first 5–7 days in microgravity and then normalized over the course of the flight. These data indicate that the gain of the aVOR is increased during active lateral gaze fixations in space flight, and show that the underlying neural activity is appropriate to produce these changes.

Introduction

The primate research program “Bion” on the biosatellite “Cosmos” was planned in the 1970s to investigate vestibular dysfunction in space, with the aim that the outcome would benefit humans traveling in space. At that time the Space Adaptation Syndrome (SAS) was observed in 30–40% of cosmonauts, but there was no possibility of obtaining direct measurements of parameters related to vestibular, proprioceptive, motor, or other dysfunction during piloted flight, and most of the information on vestibulo-oculomotor dysfunction related to microgravity was obtained during postflight testing (Uganov, 1974). Moreover, changes observed after landing could be related not only to the effects of weightlessness but also to the factors that cosmonauts experience during landing (see Section 1). To obtain direct measurements of the vestibular dysfunction in microgravity, the space capsule “Vostok,” which was originally designed for single-occupancy Cosmonaut flight and which had been used for six orbital flights, was adapted to handle two primate capsules (Gazenko and Ilyin, 1987). In this review we will refer to these experiments as Cosmos or Bion flights interchangeably.

There were three main vestibular studies in the Cosmos project. One was to study eye–head coordination and activity in the vestibular nerve, the medial vestibular nuclei (MVN) and the cerebellar flocculus associated with angular head movements in the horizontal plane during gaze shifts performed by the head and eyes to lateral targets, the gaze fixation reaction (GFR). Another project studied the sensitivity of central vestibular neurons to linear head displacements along the body axis. The third set of experiments studied the activity of leg flexor and extensor muscles during foot movements at different times of adaptation to microgravity. In the present review we will only cover the first two projects since the last project has been described in detail elsewhere (Edgerton et al., 2000).

The results presented here are based on information from many sources (Shipov et al., 1986; Sirota et al., 1987, 1988a, 1989a,b, 1990a,b,c, 1991b,c; Kozlovskaya et al., 1989, 1991, 1994; Yakushin et al., 1989, 1990, 1992. However, the amount of data presented in these publications is limited, and the majority of quantitative data was taken from “Final Reports” that were submitted by investigators to the Institute of Biomedical Problem officials at the end of each project (Sirota et al., 1984, 1986, 1988b, 1991a; Badakva et al., 1993).

Methods

Male monkeys (Macaca mulatta) of 3–5 kg were used in these studies. Their names were assigned alphabetically; the first letter of the monkey’s name corresponded to the sequential letters of Cyrillic alphabet (see Table 1). Although two primates traveled in each flight, information on vestibulo-oculomotor coordination and unit activity was not always available from both of them. Thus, although twelve animals took part in six Bion flights, valid data were obtained from only seven animals during four space flights of different durations. These results form the basis for the present report.

Table 1.

Flight numbers, times of launch, and monkeys in Cosmos flights

Cosmos flight number and date Taking off time Project number launch date Monkey name Flight duration (days)
1514 7:00 GMT BION 6 Abrek 5
12.14.83 10:00 Moscow Bion
1667 3:21 GMT BION 7 Vernyi 7
07.10.85 6:21 Moscow Gordyi
1887 12:43 GMT BION 8 Drema 13
09.29.87 15:43 Moscow Yerosha
2044 6:28 GMT BION 9 Jakonia #782 14
09.15.89 9:28 Moscow Zabiaka #2483
2229 13:40 GMT BION 10 Ivasha #6151 12
12.29.92 16:40 Moscow Krosha #7906
* 13:50 GMT BION 11 Lalik #484 15
12.24.96 16:50 Moscow Multik #357
*

At this point, the Russian Space Agency stopped assigning flight numbers to the “Cosmos” Missions.

Eye–head coordination test

The gaze fixation reaction (GFR), which is a shift of gaze onto lateral targets using both head and eye movements, is a structural unit of daily operant behavior, and the dynamic characteristics of the GFR are similar in men and monkeys (Bizzi et al., 1971, 1972). Small gaze shifts are usually performed first by an eye saccade and later by head movements. During gaze shifts larger than 20°, eye saccades are always accompanied by head movements (Tomlinson and Bahra, 1986; Phillips et al., 1995). The test was structured so that the monkey first directed its gaze toward a fixation light in front in the primary position. The target was then repositioned laterally. In response, the animal first made an eye saccade toward the target at its new location. Generally, about 20–40 ms after the beginning of the eye saccade the head started to move toward the target. Since the eye saccade was much faster than the head movement, the eye was directed toward the target first. Thus, the head was still in motion at the end of the saccade, and the head performed only about 20–30% of the total motion.

Experimental conditions had an effect on GFR parameters: if the appearance of the lateral target was predictable, the head could start an anticipatory movement first, while the animal was still fixating the centrally located target. In other cases the head could delay the eye saccade significantly (Dichgans et al., 1973; Grigaryan et al., 1986). Thus, when the gaze jumped from the central position to a visual target located 40° laterally, the total gaze displacement was 40°. However, the contribution of the eyes and the head varied from trial to trial (Phillips et al., 1995). To keep the gaze stationary on the new target, the eyes counter-rotated to compensate for the head motion (Bizzi et al., 1972). As demonstrated in monkeys with a bilateral loss of vestibular function, the counter-rotation of the eyes after the saccade could also be anticipatory (Dichgans et al., 1973). In normal animals, however, the counter-rotation of the eyes was due to activation of the angular vestibulo-ocular reflex (aVOR) (Dichgans et al., 1973). Visual feedback after the saccade onto a newly located target also affected the ocular counterrotation and provided the source for the adaptive modification of the aVOR gain. The major focus of the research was to determine the gain (eye velocity/head velocity) of the aVOR during these active gaze shifts onto target.

Although gaze shifts from one point to another are based on visual information, visual correction can occur only after the gaze has shifted to a new position. Moreover, since visual recognition has some delay, there was no visual feedback within about 80 ms immediately after the eye saccade. Therefore, the counter-rotation of the eyes reflected the current state of the aVOR gain. Since parameters of the GFR, such as amplitude and velocity of the eye, head and gaze movements, as well as counter-rotation of the eyes after a saccade, are determined by and reflect changes in sensitivity of the vestibular and proprioceptive sensors or brainstem structures, the GFR was considered a suitable reaction to study the effects of microgravity on vestibulo-oculomotor coordination.

Experimental paradigm utilized in Cosmos experiments

Gaze fixation reaction

Monkeys were trained to look at a central target and to position their heads straight ahead in the horizontal plane for 0.8 s. Head position was used as a feedback signal to trigger the next step. Targets located ±40° laterally from the center were presented for 1 s. The lateral targets were of two configurations. When the stimulus, a “C”, was presented, the animals were required to press on the lever located in front, beneath the target plate. If the animal pressed the lever within 1 s from the time the lateral conditional target appeared, it got a reward of 0.3 ml of juice. If the animal did not press the lever within the required time, or if it pressed the lever in response to the stimulus, which was an “E”, no juice was given. Additionally, the presentation of the next central target was delayed by 7–10 s. The appearance of targets on the left and right as well as the presentation of stimuli were randomized. Each program presentation was comprised of a set of 256 stimuli with 2/3 of them being conditional. This test was performed twice a day. In general, this test was accomplished within 20–25 m but, regardless of the animals’ performance, only the first 20 min of the morning session were stored on tape for analysis (Sirota et al., 1984, 1986, 1988b, 1991a).

MVN unit responses to linear acceleration

The response of MVN neurons to vertical linear acceleration was studied in each of the Cosmos 1667 to Cosmos 2229 flights. For this, the primate chair was elevated 45 mm slowly and then dropped suddenly to its original position with the aid of a spring mechanism. The total motion of the chair was 45 mm in all flights, but there was variation in the stimulus between flights. Most flight stimuli were comprised of a slow chair elevation over 8 s and a fast drop down to the original position. Peak acceleration for the upward motion was 0.14×10−4 g. This is close to the threshold for detection of linear acceleration by the vestibular system, which is ≈0.1×10−3 g for humans (Guedry, 1974). Thus, any responses observed during the elevation phase could have been due to random fluctuation or other factors. The stimuli parameters for the motion down in the drop varied on Earth and in Space. On Earth, the chair moved down over 0.6 s, and the downward pull of the spring was aided by the pull of gravity, to provide a downward acceleration of 25.4×10−3 g. In Space the chair moved over 0.9 s, to provide a downward acceleration of 11.0×10−3 g.

Surgical procedure

Two surgical approaches were used in the Cosmos experiments to implant the head holders. In the traditional method, used in Cosmos 1514, two bolts were implanted on the skull to fixate the head mount. A new technique that was minimally invasive was developed for later flights (Sirota et al., 1988a), and is described in full detail elsewhere (Yakushin et al., 2000b). EOG electrodes were implanted bitemporally to record the horizontal component of eye movements as well as above and below the left eye to record vertical eye movements.

Identification of the brain structures

Neurons recorded in the vestibular nuclei had various types of activation but most of the isolated neurons were modulated in phase with head velocity and were activated by eye position or eye velocity (Miles, 1974; Fuchs and Kimm, 1975; Keller and Daniels, 1975; Chubb et al., 1984). Units recorded in the flocculus were similar to floccular units in previous studies (Lisberger and Fuchs, 1978a,b). Some of the recorded floccular cells had complex spikes that confirmed electrode locations near Purkinje cells in the cerebellar cortex. Attempts were also made to record units in the vestibular nerves in the Bion 8–11 projects, and some preliminary data are available (Kozlovskaya et al., 1989, 1991; Correia 1998). Since there was no way to confirm that the recordings were taken from the same population of fibers on different flight days, these observations are omitted from this review.

Recorded signals and calibration

Head position in the horizontal plane was recorded with a special device placed on the center of the head-mount in the Bion 6–10 flights. The device was based on a compass principle. DC magnets were placed on either side of the primate chair at the level of the top of the head, where the device was mounted. The head position sensor was calibrated before flight. The horizontal EOG was calibrated using two assumptions based on the preflight performance: first, it was assumed that the final gaze position was equal to the angular position of the lateral target; second, under normal, preflight conditions, it was assumed that the counter-rotation of the eyes was fully compensatory during the GFR, and, therefore, that gaze (eye + head) position was stable after the eye saccade until the end of the head movement. Two channels capable of recording neural activity at frequencies ranging from 0.2 to 5 kHz were used in the Cosmos 1514. Two more channels with a frequency range from 0.2 to 10 kHz were used for unit recording in Cosmos 1667 flights, while four channels of this frequency band were used in later flights.

Electrode placements into MVN and the flocculus were based on the physiological responses of the identified units. The microelectrodes were introduced through metal guide-tubes implanted in the skull through 1 mm holes drilled through the scalp and skull in stereotaxic coordinates. Coordinates to reach MVN were P2–P4, lateral 2 mm. The flocculus was approached at the level of lateral vestibular nuclei, and the microelectrodes were tilted laterally so that they would not enter the brainstem after penetrating the flocculus. Three to four guide tubes targeted each structure. The microelectrodes were made of 80 μ tungsten wires covered with epoxy.

Data analysis

The methods of data processing varied with improving technology. Records obtained in the Cosmos 1514 flight were printed on a chart recorder. Since the amplitude and velocity of many parameters had relative calibrations, it was impossible to determine delays and durations of various GFR parameters precisely. Therefore, the results from the Cosmos 1514 flight are expressed as a percent relative to the preflight values. In all other flights, analog tapes recorded during flight were digitized with eight-bit resolution with a Motorola 6800 general-purpose mainframe computer. The channel that contained the marker of central and peripheral target presentation was digitized at 5 kHz. When the presentation of a lateral target was detected, analog signals, including the horizontal EOG, head position, lever-press and marker channel were digitized at the same frequency. Data were averaged over eight data points and stored in the computer at a 1.6 ms sampling rate for future analysis. Thus, although the data were stored at 625 Hz, each data point represented an average value of eight sequential data points and, therefore, the noise level due to the digitizing process was reduced. The following parameters of GFR were analyzed: latency, duration, amplitude and peak velocity of the eye, and head and gaze movements. There were no consistent changes in latencies and they will not be considered further.

Results: Gaze fixation on lateral targets; gaze fixation reaction (GFR)

Hypermetria of gaze

A typical saccadic gaze shift to the lateral target in preflight testing before the Cosmos 1514 flight is shown in Fig. 1A. A head movement in the same direction accompanied the eye movement. In the first inflight recording on the second day of space flight, the amplitude of the saccades was larger than before the flight, and the amplitude of head movement was approximately the same. Therefore, the gaze shift was hypermetric (Fig. 1B). Presumably, since the reward was dependent on accurate fixation of the target within one second, the animal overcame the hypermetric gaze shift after the initial period, as in Fig. 1F. Overall, the amplitude of saccades during gaze shifts performed with a single saccade in this monkey increased during flight. The increase was 11 ± 3% on day 2 and gradually increased during the flight, reaching a maximum of 42 ± 7% on day 5. Concurrently, the amplitude of head movement was smaller in flight, decreasing by 34% on flight day 2, and the head movements were still 27% lower than before flight on day 3. The head movements then normalized, and were only about 8% smaller on flight days 4 and 5. This animal performed the lateral gaze shift with one saccade before flight, using multiple saccades only 4% of time (Fig. 1C). The multisaccadic gaze shifts increased to 36% on the second day of space flight. The number of gaze shifts made with multiple saccades was highest on day 2 and then decreased to 14% on flight days 4 and 5 (Fig. 1C).

Fig. 1.

Fig. 1.

A–C, Gaze fixation reaction onto a target located 40° to the right, performed by monkey Abrek before (A) and on the second day (22 h) of space flight (B). The data from each day had the same gain, and therefore the data could be compared. C, Percent of gain fixation reaction performed with corrective saccade before and during flight. D–F, Gaze fixation onto lateral targets performed by monkey Drema before (D) and during the first (E) and sixth (6) day of flight. The traces in D were reversed to facilitate comparison with E and F. Adapted from (Sirota et al., 1984; Shipov et al., 1986; Kozlovskaya et al., 1989).

Parameters of the GFR were similar in the monkey studied during the Cosmos 1887 flight. The gaze amplitude, which was 40.2 ± 6.9° before flight, became hypermetric in space, going from 46.0 ± 8.5° on the first day, to 58.3 ± 7.0° on the 5th day. The gaze amplitude was slightly smaller (51–52°) when tested on days 8 and 10. Examples of these gaze shifts are shown in Fig. 1DF. Before flight, gaze was stable on the lateral target over the entire period of head movement (Fig. 1D, dashed line). In flight, gaze was hypermetric, mostly due to the increased amplitude of the saccades, but gaze came back onto the target after the initial overshoots (Fig. 1E, F, dashed lines).

In Cosmos 2044, the gaze movements to the 40° lateral targets before flight were 38.0 ± 0.4° and 37.0 ± 0.6° in the two monkeys (Fig. 2). On day 2 in space, the gaze amplitudes were 47.0 ± 1.3° in the monkey Jakonia (Fig. 2A) and 48.0 ± 1.9 in monkey Zabiaka (Fig. 2B). The gaze amplitudes normalized, however, within the next several days in both animals. Detailed analysis revealed substantial differences in the source of observed changes. Although both animals had hypermetric gaze on day 2, the gaze overshot the target due to larger saccades in Jakonia, while the overshoot was due to larger head movements in Zabiaka.

Fig. 2.

Fig. 2.

Parameters of gaze fixation on the lateral targets performed by monkeys Jakonia (A) and Zabiyaka (B) during flight of Cosmos 2044.

In the Cosmos 1667 and 2229 flights, most gaze shifts were associated with multiple saccades. The amplitude of the associated head movements was decreased (Gazenko and Ilyin, 1987; Sirota et al., 1987). Multiple saccades were not characterized quantitatively, but the gain of the compensatory aVOR was increased (see below). Thus, similar to the other flights, the lateral gaze displacements during the Cosmos 1667 and 2229 flights were also hypermetric.

In summary, gaze shifts to lateral targets in each of the six animals became hypermetric in the first few days of flight. This was observed whether the monkeys made the gaze shift in single or multiple saccades. In five of the six monkeys, the gaze overshoot was mainly due to an increase in the amplitude of the saccades, while in one animal it was due to an increase in the amplitude of the head movements (Fig. 2B). Thus, for successful visual fixation of target during head movements, the hypermetria had to be compensated for either by a corrective saccade or by a change in the gain of the aVOR (Fig. 1F).

Increase in the gain of the angular VOR (aVOR)

The gain of the aVOR was defined as the ratio of eye velocity to head velocity during counter-rotation of the eyes after the animals had made a saccade onto target. In Cosmos 2044, the instantaneous aVOR gain was studied as a function of time, starting from the end of the eye saccade over a 128 ms time period. When the eyes were stationary just after the saccade, the aVOR gain was zero. As counter-rotation began, the gain gradually rose. Under normal conditions the aVOR gain is 1.0, so the eye velocity is equal to head velocity over the counter-rotation period.

Nine superimposed gain curves obtained before flight in monkey Zabiaka are shown in Fig. 3A. The aVOR gain increased to unity within the first 30 ms after the saccade and then remained stable while the head was in motion. In most cases, the head movements ceased after 80 ms (Fig. 3E). Consequently, the aVOR gains were calculated as average values over the time interval from 32–64 ms after the initial saccade. Average instantaneous gain curves based on 30 responses before flight (Fig. 3B) were similar to those in Fig. 3A.

Fig. 3.

Fig. 3.

Gain of the aVOR measured during eye counter-rotation during the gaze fixation task. A, Nine superimposed instantaneous gain curves obtained in monkey Zabiyaka (Cosmos 2044) before flight. The arrows in A and the vertical dashed lines in B–E indicate the regions where average values were measured. F, Individual aVOR gains for each animal tested during space flight. G, Average (±1 SD) gains over space flight for the entire series, based on the individual responses shown in F.

In flight there were substantial changes in aVOR gains. As shown in Fig. 3C, the gain of the aVOR increased to about 1.5 on the first recording of day 2 (Fig. 3C) and remained at this level until day 8 (Fig. 3D), when the increase became even larger (≈2.0). The gain was still about 1.5 on day 14 (Fig. 3E). Changes in the gains of the aVOR were similar during gaze shifts in either direction and were combined to obtain the average gain changes for this monkey (Fig. 3F, filled circles). The aVOR gain was also increased when the other animal of this flight, Jakonia, was tested for the first time in space on day 3 (Fig. 3F, filled squares). The gain increase was smaller subsequently, but was present over the entire flight.

The average gain values obtained from the instantaneous gain curves were compared to the aVOR gains obtained from taking the ratio of eye and head velocities at arbitrary points during the counter-rotation. The average aVOR gains were the same when measured with either method (Sirota et al., 1991b). Thus, it was possible to compare the aVOR gain measurements in the different Cosmos projects. Individual gain curves for each of the monkeys in this report are shown in Fig. 3F. There were individual differences, but as a group, there was a substantial increase in the aVOR gains that persisted over the entire flight (Fig. 3G).

In summary, the general conclusion is that gaze became hypermetric upon entry into space on each of the Cosmos flights and that the positional errors generated by this gaze overshoot were compensated for by an increased gain of the aVOR. Although both of these changes could have occurred independently, since they occurred in parallel, it is more likely that one was primary, while the other was an adaptive response to the primary change.

The angular acceleration that activates the semicircular canals is the same on Earth and in space. Accordingly, the gain of the passive aVOR induced by steps of velocity and by voluntary sinusoidal head oscillation in darkness were not affected in microgravity (Benson et al., 1986; Cohen et al., 1992; Clarke et al., 2000). If the hypermetric gaze was primarily due to exposure to microgravity, then the alteration in aVOR gain was a simple compensation for the positional error, driven by the visual feedback. However, there are reasons to question this explanation. First, the source of the hypermetric gaze varied among animals. In one, it was due to an increase in the amplitude of head movements (Fig. 2B), while in the others, it was due to the increase in the amplitude of the saccades. Of interest is that similar increases in gaze amplitude have been observed in both human and monkeys after water immersion (Barmin et al., 1983; Kreidich et al., 1983; Badakva et al., 2003). In monkeys the hypermetric gaze was due to an increase in saccade amplitude (Badakva et al., 2003), while in humans the amplitude of the head movements increased (Barmin et al., 1983; Kreidich et al., 1983). There was no change in the acceleration of gravity in these experiments, yet the changes were similar to those during space flight.

An alternate explanation is that the increase in the gain of the aVOR gain was the primary event. Similar changes in aVOR gain were also observed after water immersion (Barmin et al., 1983; Kreidich et al., 1983; Badakva et al., 2003), and as in the Cosmos 1667 flight, the first gain changes were observed after only two hours of immersion. Since changes in gravity were not a factor in these experiments, changes in proprioceptive inputs could have contributed to or been responsible for producing the gain changes. If the aVOR gain changes were the primary even, then parameters of the GFR should be different if the eye saccade was not accompanied by head motion. Kozlovskaya and colleagues demonstrated in cosmonauts tested before and after space flight that there are two types of the adaptive changes in GFR. One group had changes in the amplitude of the saccades and in aVOR gains, similar to those observed in the monkeys. The second group was comprised of spacecraft commanders, e.g., professional pilots. They performed gaze shifts in two stages: first by a saccade onto target and then by a head movement, which followed the saccade. In the pilots, changes in their aVOR gains were similar to those described above. Since the amplitude of the saccades during the gaze shift was accurate within ±3°, there was no visual/vestibular mismatch that could have driven the changes in the aVOR gains (Kozlovskaya et al., 1985).

An alternate mechanism could also have been responsible for the changes in the gain of the aVOR. It was recently demonstrated that adaptive changes of the aVOR gain are a function of head position with regard to gravity (Tiliket et al., 1993; Yakushin et al., 2000a, 2003a,b, 2005). Thus, “normal” aVOR gains during active head movements may only exist under the level of gravity and/or proprioception in which the aVOR gains were adapted, and a change in gain of the aVOR due to insertion into microgravity could have been the primary change that produced the changes that were observed in microgravity.

If there were changes in the gain of the aVOR, there should be associated changes in the cellular activity in the vestibular nuclei and/or flocculus, which produced the adaptive changes in aVOR gain ((Lisberger, 1994; Lisberger et al., 1994a,b), see Ito (1984) for review). Unit activity was recorded in the vestibular nuclei and flocculus during each space flight and is considered in the next section.

Neural activity in the vestibular nuclei and flocculus during space flight

Activity of a single lateral canal-related neuron in the right MVN of monkey Vernyi (COSMOS 1667) during sinusoidal head/body oscillation before flight is shown in Fig. 4A. The discharge rate increased in phase with ipsilateral head velocity (Fig. 4B). Therefore, this cell was a type I unit.1 When this unit was well isolated from the background, the electrode was fixed at this location. Over time, this electrode recorded several neurons simultaneously. The multiunit activity recorded before and after the flight increased with ipsilateral rotation and had a similar phase relationship to head velocity (Fig. 4D) as the neuron in Fig. 4A. The electrodes over the various Cosmos flights were implanted in MVN in the region of type I units.

Fig. 4.

Fig. 4.

Activity of the lateral canal-related type I neuron recorded the right medial vestibular nuclei in the monkey Vernyi (Cosmos 1667). A, Single unit recording at the site where one of the MVN electrodes was installed. Head position down is rotation to the right (ipsilateral). B, Poststimulus histogram for the unit shown in A. Traces below show head position and head velocity during sinusoidal rotation. C–D, Integrated unit activity recorded from the same electrode before (C) and after (D) seven days of the space flight. Note that the modulation in unit activity increased peaking just before the ipsilateral (rightward) head velocity had reached maximum. The head oscillation shown in A–D was driven manually with approximate frequencies 0.45 Hz (A, B), 0.5 Hz (C) and 0.4 Hz (D).

Multiunit activity recorded from three of four of the implanted electrodes in the two animals in Cosmos 1667 was of good quality. An example of a recording during a gaze shift to the right during flight is shown in Fig. 5A. Single neurons, shown as standard pulses, could be separated from the background (Fig. 5B). The quality of separation was similar for each flight day, although it was not certain that the same neurons were analyzed throughout the flight. Before flight, the peak activation occurred approximately at the time when ipsilateral head velocity reached a maximum (Fig. 5C, Before). The unit activity did not decrease relative to the resting discharge rate (white dashed line) in association with contralateral head velocity. The profile of activation by ipsilateral head velocity was the same over all flight days. The amplitude of peak activation before flight (27±4 imp s−1) was comparable to the peak activation recorded during the second hour of space flight (23±6 imp s−1, day 1). This activation became larger on flight days 2–4 (50±8 imp s−1, day 2) and then decreased to normal on days 5–6 (25±3 and 22±3 imp s−1, respectively). Thus, the activation was twice the normal value after 26 h in space (day 2). The changes were substantial over the next 2 days and then normalized. Data from this neuron are summarized in Fig. 6F (filled symbols). There was no significant change in the activity recorded during gaze shifts to the right after 2 h of space flight (day 1), but the activity gradually increased to a maximum on day 4, and returned back to normal for the rest of the flight.

Fig. 5.

Fig. 5.

A, Sample of multiunit activity recorded in the right vestibular nuclei in monkey Vernyi (Cosmos 1667) during the gaze fixation reaction onto the target on the right. The recording was obtained from the same electrode at the same location as in Fig. 4. B, Activity of the largest neuron from a sample similar to that shown in A and converted to standard pulses. C, Poststimulus histograms of this unit recorded at different times in flight. Thirty head movements of similar profile and amplitude were identified for each day. Head motion to the right and back to the center was divided into eight bins. An additional eight bins were used to characterize the data from before and after head motion. The idealized head position and head velocity are shown under each histogram.

Fig. 6.

Fig. 6.

A–C, Integrated (30 ms) multiunit activity from the right MVN recorded during angular head movement, when animal Vernyi performed gaze fixation onto the right lateral target, before (A), and on the second (B) and seventh (C) day of space flight (Cosmos 1667). D–F, Peak integrated MVN activity recorded on different days of space flight in monkeys Drema and Erosha (D, Cosmos 1887), Jakonia and Zabiaka (E, Cosmos 2044) and Vernyi (F, Cosmos 1667). G–H, Changes in flocculus activation during angular head rotation in the Cosmos 1887 (G) and Cosmos 2044 (H) flights. MVN-1 and MVN-2 (D) represent recordings from different sides of the brain. The location of the electrodes in the left or right MVN of the flocculus for Cosmos 1887 and Cosmos 2044 flights was not identified in the reports (Sirota et al., 1988b, 1991b; Kozlovskaya et al., 1989). I, Average activity in MVN (solid line) and the flocculus (dashed line) for animals tested in the COSMOS flights. D–I are normalized to the preflight date.

The profile of the integrated multiunit activity was similar when multiunit activity recorded by the same electrode was integrated (Fig. 6AC). That is, activation before flight (Fig. 6A) was similar to that on day 7 (Fig. 6C), and the increase in unit activity was larger on day 2 (Fig. 6B). The integrated activity from the multiunit recordings over the entire flight is shown in Fig. 6D (open symbols). Activation on flight day 1 after 2 h was the same as the preflight activity. This activity significantly increased on flight day 2 and then returned to normal by days 5–6 (Fig. 6F). The difference between the single and integrated multiunit recordings was presumably due to variation in response of the neurons in the vicinity of the recording electrode.

The multiunit activity in MVN was also studied in four other animals. The two animals in Cosmos 1887 had two electrodes implanted in MVN (Fig. 6D) and the two animals in Cosmos 2044 flight (Fig. 6E) each had one electrode in MVN. The sensitivities recorded in Cosmos 1887 flight were maximal on day 3 for all four electrodes and then decreased to normal in three of the four electrodes (Fig. 6E, filled circles). Changes in the sensitivities of the MVN neurons in the monkeys of Cosmos 2044 flight were more robust. The sensitivities increased significantly on day 3 and stayed high until day 8 when they began to normalize. In the animal Jakonia, the sensitivity stayed above the normal even on day 13 (Fig. 6F, filled symbols).

Multiunit activity was recorded in the flocculus from one electrode in each of the same four animals. In all cases the change in the sensitivity was maximal on the first day of flight (Fig. 6G, H). In two animals, the activity normalized by the middle of the flight (filled symbols), while in other two, it stayed above the norm until the last day of flight (Fig. 6G, H, open symbols).

A summary of all multineuronal recordings from the Cosmos flights is shown in Fig. 6I. Overall the sensitivity of the neural activity in both the vestibular nuclei and flocculus was maximal in the earlier days of flight, with the rise in activity occurring earlier in the flocculus than the MVN neurons. There was a striking similarity between the rise in activity of the flocculus (Fig. 6I, dashed line) and MVN multineuronal activity (Fig. 6I, solid line) and the increases in aVOR sensitivity shown in Fig. 3G. The flocculus activity tended to rise earlier and persist longer than the MVN activity, but both were increased over the two weeks of flight. Thus, the changes in neural activity in MVN and flocculus during space flight mirrored the changes in aVOR sensitivity during the gaze fixation reaction. Presumably, the flocculus units were involved in the learning that changed the gain of the aVOR, while the increase in unit sensitivity in MVN to head rotation reflected the actual changes in gain in the compensatory processes.

Response of MVN units to linear acceleration in space

The first inflight recordings of central vestibular neurons during otolith stimulation in the Cosmos 1667 project utilized the same population of neurons in the right MVN of monkey Vernyi that was studied during angular rotation (Figs. 4, 5, 6AC, F). A sample multiunit activity during otolith testing on day 1 is shown in Fig. 7A, and associated single unit activity in Fig. 7B. The stimulus cycle was divided into four phases for analysis. The spontaneous discharge rate (Phase 1) was obtained from a 1 s time period before each elevation of the chair. Unit activity during the elevation (Phase 2) and rapid drop (Drop, Phase 3) were taken as average values.2 Additionally, activity was also utilized over a 1 s period immediately after the drop had terminated (Stop, Phase 4). Data were first expressed in imp s−1 and then normalized to activity in Phase 1 of each day. The bottom traces (Chair) in Figs. 7A, B, show the time intervals for each phase.

Fig. 7.

Fig. 7.

A, Multiunit recording in the right MVN of monkey Vernyi (COSMOS 1667) during linear motion along the long body axis. Phase-1, Resting activity before stimulation; Phase-2, Slow elevation of the chair up; Phase-3, Fast movement down (Drop); Phase-4, Activity immediately after the Drop. B, Activity of a single unit discriminated from the multiunit record. The vertical eye position record indicates that there was up-beating nystagmus during Phase-3. C, Activity of the same unit in different days of flight normalized to the activity in Phase 1 on that day. D, Activity of the unit in Phase-3 on different days of space flight.

The resulting histograms for each flight day are shown in Fig. 7C. The first significant changes in the drop phase occurred on the first day after 2 hours of space flight. This activity normalized on days 2 and 3, but then increased again, reaching a much higher level (Fig. 7C, D). Sensitivity of the activity for the Drop in Phase 3 for each day is shown in Fig. 7D. The first significant changes were observed in the first day of flight. Activity was near normal on flight days 2 and 3 and then increased again on days 4–5. The direction of linear acceleration was opposite during the Drop and the Stop phases, but there was no difference between the two responses on any flight day. Since the head was not fixed during the Stop, it is not known whether the head continued to pitch at the time of the Stop, which could explain this apparent disparity. Therefore, the activity associated with the Stop Phase will not be considered further in the analysis.

Integrated multiunit activity from the second animal in the same flight (Gordyi) is shown in Fig. 8AC. Before the flight, there was a brief increase in activity during the Drop (Fig. 8A). On the second day of flight there was a significant increase in activity during the Drop (Fig. 8B). The activity increased in response to the acceleration phase and then decreased to normal during the chair deceleration. The activity during the entire period on day 7 was more irregular than the other days (Fig. 8C), and the response to the Drop was again brief. Integrated activity recorded from both animals in the Cosmos 1667 flight is shown in Fig. 8D. The sensitivity of these MVN units was not changed on day 1, but was increased in two of the three electrodes on day 2. The activity increased further up to day 5, and then normalized.

Fig. 8.

Fig. 8.

A–C, Integrated (30 ms) multiunit activity recorded in monkey Gordyi during linear stimulation along the longitudinal body axis recorded before (A) on the second (B) and seventh (C) day of flight. D–E, Average multiunit activity in MVN in Phase-3 (see Fig. 7) on different days of the Cosmos 1667 (D) and Cosmos 2044 (E) flights. Multiunit activity in Phase-3 normalized to the activity observed before stimulation in Cosmos 1667 (D) and to the level of activation in Phase-3 recorded before flight in Cosmos 2044 experiment (E). Note that multiunit activity recorded in the right MVN of monkey Vernyi was not modulated in this test, but the single unit that was selected from this record (Fig. 7) was well modulated by the linear acceleration.

Changes in the sensitivities of the MVN neurons in the monkeys Jakonia (Fig. 8E, open circles) and Zabiaka (Fig. 8E, open squares) from Cosmos 2044 were similar to those shown in Fig. 8D. The sensitivities gradually increased reaching maximal values on day 6 and then declined, although they were still above the baseline on the last day of flight (day 13). Thus, changes in the sensitivity of the MVN neurons to vertical linear acceleration mediated by the otoliths were similar in animals from the Cosmos 1667 and Cosmos 2044 flights. The sensitivity to linear acceleration gradually increased in space, reaching a maximum at days 5–6 and then decreasing toward normal values. The peak increases in sensitivity for the MVN neurons in Fig. 6D, E in response to angular acceleration during the gaze fixation reaction were between 300 and 600%, whereas the increases in sensitivity during linear acceleration were smaller, within 200–250%. Thus, the general pattern of response was similar to that obtained from angular acceleration, but the magnitude of the response to linear acceleration was smaller. This could represent a difference in response to angular and linear accelerations or could reflect a difference in the magnitude of convergence of the otolith and canal signals onto these neurons.

The responses to linear acceleration produced by sinusoidal oscillation along the body vertical axis in the Bion 11 Project were very similar to those observed in the Bion 9 (Cosmos 2044) flight. The multiunit activity of the neurons recorded in MVN in each animal was in phase with upward acceleration in monkey #484 and with downward acceleration in monkey #357 (Badakva et al., 2000). In both cases, the sensitivity to linear acceleration increased only slightly on the first recording on Day 2, and reached a maximum on Days 4–6. Sensitivities then decreased but were still above normal up to the last day of flight.

Discussion

The data from the Cosmos flights show that the sensitivity of central vestibular neurons in MVN to both angular head rotation and vertical linear motion was affected by microgravity. In general, the sensitivity of these neurons increased in the earlier days in Space and then gradually normalized. In some instances changes were similar for several populations of neurons recorded on both sides of the brainstem from the same animal (Fig. 6D, E). In other cases, although average activity of the recorded neurons had similar changes in sensitivity during adaptation to microgravity (Fig. 6F, open symbols), the changes in sensitivity of a single unit could differ from the changes observed in the remaining population of units. A striking finding was that the observed changes in neuronal sensitivity were qualitatively similar to the changes observed in the aVOR gains and occurred over the same time course. Changes in sensitivity of the floccular neurons to the angular rotation were more uniform than the changes in MVN activity, presumably, because the flocculus was responsible for producing these adaptive changes.

Changes in sensitivity of the neuronal populations in the vestibular nuclei to the otolith stimulation were also relatively uniform and had approximately the same time course as the sensitivity to angular acceleration. The sensitivity to linear acceleration gradually increased, reaching a maximum by the end of the first week in space (Fig. 7D and Fig. 8D, E). This was different from the changes in sensitivity of the same neuronal population to angular rotation, which increased earlier in flight and was normalized by the time the otolith sensitivity had reached a maximum (Fig. 6I). This was somewhat surprising, since it would be expected that microgravity would affect otolith and not canal sensitivity. A majority of direct projections from otolith afferents go to the lateral and descending vestibular nuclei (Büettner-Ennever, 1999), but there are canal-sensitive neurons with some otolith sensitivity in MVN (Markham and Curthoys, 1972), which could serve a different purpose than maintaining balance or supporting the linear VOR. Otolith information is not necessary to induce changes in the angular VOR gain (Crane and Demer, 1999). As recently shown, however, the head position with respect to gravity in which the aVOR gain was adapted is expressed subsequently in changes in aVOR gain in every head position (Yakushin et al., 2000a, 2003a,b, 2005). Therefore, the otolith signals could serve as a gravitational context for adaptation of the aVOR gain in specific head positions, and the changes in otolith sensitivity could be a reflection of changes in this gravitational context.

SECTION 3: NASA–RUSSIAN MONKEY EXPERIMENTS ON THE ANGULAR AND LINEAR VESTIBULO-OCULAR REFLEX

Abstract

The angular and linear vestibulo-ocular reflexes (aVOR and lVOR) of four rhesus monkeys were recorded before and after the 1988 and 1992–1993 Cosmos Space Flights 2044 and 2229 (Table 1). Two animals flew in each mission for approximately two weeks. Eye movements, induced by rotation with steps of velocity about a vertical axis, by constant velocity rotation about axes tilted from the vertical (off-vertical axis rotation, OVAR), and by horizontal and vertical translation were recorded binocularly with scleral search coils in two- and three-dimensions. Single unit recordings were also taken from semicircular canal afferents before and after flight.

Compensatory eye movements produced by the angular VOR (aVOR).

Gains of semicircular canal-induced horizontal and vertical aVOR were unaffected in both flights, although the gain of the roll aVOR was diminished. Up/down asymmetries of vertical nystagmus present before flight were reduced for seven days after flight.

Activity of primary lateral canal afferents after space flight.

The mean gain for nine different horizontal canal afferents, tested on the first postflight day of Cosmos 2044 with steps of velocity and sinusoidal rotation, was nearly twice that of 20 horizontal canal afferents similarly tested during preflight and postflight control studies. Adaptation of the afferent response to passive yaw rotation on the first postflight day was also greater. After the Cosmos 2229, however, afferent gains were reduced.

Spatial orientation of the aVOR.

Spatial orientation of the aVOR was altered in two of the four monkeys after flight. In one, the time constants of postrotatory nystagmus, which had been shortened by head tilts with regard to gravity before flight (“tilt dumping”), was unaffected by the same head tilts after flight. In another animal, eye velocity, which tended to align with gravity before flight, moved closer toward a body axis after flight. This shift of orientation had disappeared by seven days after landing.

Compensatory eye movements produced by the linear VOR (lVOR).

The gain of the high frequency compensatory lVOR was reduced for naso-occipital linear acceleration in one monkey, but maintained in a second monkey. Gain changes in the first animal lasted for 17 days after landing.

Orienting eye movements produced by the lVOR.

The gain of the low frequency lVOR was tested using OVAR. Ocular counter-rolling (OCR) was reduced by about 70% during both the dynamic tilts experienced during OVAR and in response to static tilts. Similarly, modulation in vergence, in response to low frequency, naso-occipital linear acceleration during OVAR was reduced by over 50%. These changes in orienting eye reflexes persisted for 11 days after recovery.

Orientation of eye velocity induced by velocity storage.

Steady state yaw axis horizontal eye velocities induced by OVAR were unaffected by space flight. The orientation of optokinetic after nystagmus (OKAN) and of vestibular nystagmus was altered, moving closer to a body than a spatial axis when tested shortly after landing in one animal.

Conclusion.

There were both short and long term changes in otolith-ocular reflexes after adaptation to microgravity in both monkeys in the Cosmos 2229 flight, although horizontal and vertical semicircular canal-induced responses of the angular VOR to rotation were largely unaffected. The roll aVOR gain was also reduced. All of the reductions were greater in one animal (7906) across all tests. A comparison with data from astronauts suggests that maintenance of gain of both compensatory and orienting otolith ocular reflexes may depend on continuous exposure to linear acceleration during flight. Presumably, in future long duration space flights, this could be provided by centrifugation.

Introduction

The vestibular system is composed of two subsystems. One, comprised of the semicircular canals, senses angular acceleration of the head and generates compensatory eye movements that stabilize gaze during head and body movement over the angular vestibulo-ocular reflex (aVOR) (see Raphan and Cohen, 2002; Cohen and Gizzi, 2003; Cohen and Raphan, 2004 for review). Since the natural angular motion that excites the aVOR is essentially turning on a head- or body-centric axis, the horizontal aVOR would not be expected to change dramatically in a different gravitational environment. The second component of the vestibular system, however, the otolith organs, comprised of the saccules and utricles, sense both head orientation and head linear translation. The altered acceleration profiles experienced in microgravity should induce very different activation profiles in otolith afferents that could initiate morphological and behavioral adaptation of the vestibulo-ocular and vestibulo-spinal reflexes that depend on gravity. Thus, it would be expected that there might be changes in ocular counter-roll (OCR), vergence and spatial orientation after adaptation to microgravity but that the angular VOR would be less affected.

The linear vestibulo-ocular reflex (lVOR) can be further separated into high and low frequency components, using approximately 0.3 Hz as the divide between the two. The compensatory reflex provides ocular compensation against high frequency head translations (Schwarz et al., 1989; Hess and Dieringer, 1991; Paige and Tomko, 1991a,b; Schwarz and Miles, 1991; Raphan and Cohen, 2002), and is used to maintain fixation on near targets during translation (Paige and Tomko, 1991a; Schwarz and Miles, 1991; Maruta et al., 2001) or in response to centripetal acceleration generated by turning corners (Imai et al., 2001). Vergence in response to high frequency linear acceleration along the naso-occipital axis is also compensatory, and supports fixation of near targets when moving forward (Paige, 1991; Dai et al., 1996). There are also low frequency orienting otolith-ocular responses that tend to maintain the position of the retina in relation to the spatial vertical (Cohen et al., 2001). These include horizontal, vertical and torsional shifts of the eyes, OCR, and sustained vergence in response to head tilts with regard to gravity (see Dai et al., 1996 for review). Finally, angular eye velocity induced through activation of a central vestibular system known as “velocity storage” by the visual, vestibular and/or somatosensory systems, tends to orient to gravity or to the GIA when the GIA is tilted with respect to the head (Dai et al., 1991, 1992).

In the pre- and postflight experiments described in this section, scleral search coil measurements of eye movements in response to controlled vestibular and visual stimulation were utilized in pre- and postflight experiments. The purpose was to demonstrate the effects of adaptation to microgravity on return to the 1 g environment of Earth. Experiments were also done on semicircular canal afferents to determine if the exposure to microgravity had significantly changed afferent activity after adaptation to microgravity.

Methods

Nineteen juvenile rhesus monkeys (Macaca mulatta) were candidates for the two Cosmos Biosatellite Flights. Of these, four animals were chosen for flight; the others served as controls. Monkeys 782 and 2483 flew in Cosmos Flight 2044. They were launched on 9/15/89 and recovered on 9/29/89 (Table 1). Animals 6151 and 7906 flew in Cosmos Flight 2229. These animals were launched on 12/29/92 and recovered on 1/10/93. Testing extended for 5 and 11 days postflight, respectively. In space, the monkeys sat in a capsule, 60 cm in diameter, in fur-lined chairs. The compartments that held the primate chairs were separated from each other, but the animals were within sight of one another. Their trunks were restrained, but their heads, arms and legs were free. The monkeys performed behavioral testing in space, moving their head and eyes toward lateral visual targets (see Section 2). The status of the animals was monitored by downlinked video, along with continuous recording of a wide range of other control signals from the capsule, including temperature, humidity, and food and water intake. Monkeys not chosen to fly were housed in comparable quarters on ground and served as controls. The experiments conformed to the Principles of Laboratory Animal Care (NIH Publication 85-23, Revised 1985), and were approved by the appropriate Institutional Animal Care and Use Committees.

Pre- and postflight testing

During experiments, the monkeys sat in a primate chair with their heads fixed to a plastic frame that held a square field coil, 25.4 cm on a side. The same primate chair and coil box was used in studies of high frequency linear oscillation. Yaw (horizontal), pitch (vertical) and roll (torsional) eye movements were recorded through two search coils, which were attached to the front and the top of the left eye. A frontal plane coil was also implanted on the right eye of the Cosmos 2229 monkeys. Voltages associated with eye position and with the position and velocity of the various axes were recorded through analog filters with a bandwidth of DC to 40 Hz. Eye positions and velocities were calibrated by assuming that the animals accurately tracked visual surround movement during rotation in light at 30°/s. Movements to the right and up caused upward trace deflections. Roll velocities were assumed to have a gain of 0.6. Eye movements were not recorded in the studies of afferent activity in the vestibular nerve.

Two multi-axis vestibular stimulators and three vestibular/oculomotor laboratories were transported from the United States to the Institute of Biomedical Problems in Moscow for these experiments. The apparatus and experiments are fully described in previous publications and reports (Cohen et al., 1992; Correia et al., 1992; Tomko et al., 1993; Dai et al., 1994, 1996). In brief, the apparatus shown in Fig. 9A was used to study the angular VOR (aVOR), optokinetic nystagmus (OKN), optokinetic after-nystagmus (OKAN), and the response to off-vertical axis rotation (OVAR). The response to angular acceleration was given by rotating the animals positioned in separate tests so that their yaw, pitch and roll axes were aligned with the spatial vertical. Optokinetic nystagmus (OKN) was induced by rotating the light-tight OKN shell around the animal’s yaw axis with the yaw axis upright or in tilted positions. Off-vertical axis rotation (OVAR) was given by rotating the animals around a tilted yaw axis. The response to static tilts was tested by incrementally rotating the circular spine around the horizontal axis.

Fig. 9.

Fig. 9.

A, Four axis vestibular and optokinetic stimulator for testing the aVOR, and for inducing OKN and OKAN and OVAR. Also shown are the primate chair and coil field apparatus used to activate the scleral search coils when recording eye position and eye movement. The same coil box and primate chair was also utilized in the linear oscillation apparatus. B, Portable linear sled for high frequency linear oscillation. A gimbaled, light-tight Specimen Test Container sat on a carriage supported by air bearings and “floated” on ceramic rails. The linear track was situated on a gantry that could be repositioned to give translation along earth-horizontal (Ba), oblique (Bb), or earth-vertical (Bc) axes. Stimuli were given in darkness, in a subject-stationary lighted visual surround (VSLVOR), or while viewing the visual surround that could move relative to the subject (VLVOR).

For tests of high frequency linear acceleration, the animals were oscillated on a linear sled, specially constructed at the NASA-Ames Research Center (Fig. 9B). Animals sat in a Specimen Test Container and moved along a linear track in Earth-horizontal (Fig. 9Ba), oblique (9Bb) or dorsoventral (9Bc) directions. In Ba, the animals were upright and in Bc they were either prone or supine. Motion was delivered along the interaural, naso-occipital, and dorsoventral axes as well as along intermediate oblique axes. lVORs were studied during 1.0 and 5.0 Hz Earth-horizontal head motion in darkness and while viewing a head-fixed (VSLVOR) or an earth-fixed (VLVOR) visual scene.

Afferent neural responses from the horizontal semicircular canals were tested by rotating the animals sinusoidally or at a constant velocity about a spatial vertical axis (not shown). To test potential sensitivity of the canal units to tilt before and after flight, the animals were also pitched along the naso-occipital axis.

Results

Compensatory eye movements from the angular VOR (aVOR), horizontal aVOR

For studying the gain of the aVOR, monkeys were tested with short (5 s) steps of constant velocity rotation from 30°/s to 180°/s in 30°/s intervals in darkness (Fig. 10A). For studying the time constant of the aVOR, monkeys were rotated at 60° /s in darkness to produce per-rotatory nystagmus. When the nystagmus died away, the animals were stopped to produce postrotatory nystagmus (Fig. 10A, B). The animals were subsequently rotated in the opposite direction and stopped. The slow phase eye velocities of the two per- and two postrotatory nystagmus profiles were fitted by single exponentials to extract the central vestibular time constants, and were averaged to generate a mean time constant. The gains (eye velocity/head velocity) of the response to short steps measured the status of the high frequency aVOR, and the time constants gave the state of the central velocity storage mechanism, which provides the low frequency characteristics of the aVOR and counters postrotatory nystagmus (see Raphan and Cohen, 2002 for review).

Fig. 10.

Fig. 10.

A, Horizontal eye position (H POS) and eye velocity (H VEL) in response to 5 s steps of velocity (rotation about a vertical axis) from monkey 2483 after recovery in the Cosmos 2044 flight. Eye positions and eye velocities to the right are up in this and subsequent figures. The changes in yaw position of the animal, which were recorded by a potentiometer that reset every 360°, are shown in the third (YAW POS) trace. Downward movement of the trace is rotation to the left. The rotations were in darkness. The surround was lighted (PHOTO CELL) between velocity steps to extinguish any nystagmus that remained after the rotations. B, C, Horizontal slow phase velocities induced by steps of velocity as in A. The induced velocities were close to the velocity of rotation up to 180°/s and were not different before and after flight.

The induced horizontal aVOR slow phase velocities were close to stimulus velocities up to 120°/s for control monkeys, and fell slightly for stimulus velocities of 150°/s and 180°/s (Fig. 10B, C). Linear, least square regressions were used to characterize each set of pre- and postflight data. Slopes, intercepts and correlation coefficients were similar for the pre- and postflight data for both 782 (Fig. 10A) and for 2483 (Fig. 10B), and the data were not significantly different from the group means of the control pool. During the Cosmos 2229 Flight, horizontal aVOR gains were pooled for rotation to the right and left, since there was no difference between them. The preflight and postflight gains were the same (Dai et al., 1994). Similarly, horizontal aVOR time constants were similar before and after flight. The mean aVOR time constant of 782 on three days of testing, about two months before flight was 22.6±7.9 s. Pooled postflight day 1 and day 4 time constants were 22.6±9.2 s and 18.8±2.1 s. These means did not significantly differ from each other. Though not significant, the reduction in time constant on postflight day 4 was likely due to habituation due to repeated testing. These findings confirm findings in humans in a NASA–ESA Spacelab Flight that indicated that 14 days of exposure to microgravity had not affected the aVOR gain (Benson and Vieville, 1986). Similarly, the time constant of the horizontal aVOR was unaffected in the NASA IML Shuttle Flight in 1992 (Oman and Balkwill, 1993).

Vertical and ROLL aVOR

Both flight and control monkeys in the Cosmos 2229 mission had an asymmetry of the vertical aVOR before flight when they were rotated on their side in pitch around a vertical axis (Fig. 11A). This stimulus only activates the vertical canals in contrast to pitch about a horizontal interaural axis while upright, which excites both the vertical canals and otolith organs. The mean gain for upward slow phases of vertical eye velocity before flight was 0.96 ± 0.03, and the mean downward gain was 0.75 ± 0.04 over a velocity range of 30 to 90°/s (Dai et al., 1994). In the first postflight test, there was a 7.3% decrease in the gain of the upward aVOR to 0.90 ± 0.03, and a 7% increase in the gain of the downward aVOR to 0.82 ± 0.03 (Fig. 3A). These differences were small but statistically significant. Thus, the increase in the gain of the downward aVOR was at the expense of a decrease in gain for the upward aVOR.

Fig. 11.

Fig. 11.

A, Averaged gains of the vertical VOR before and after Cosmos flight 2229 for monkeys 6151 and 7906. The animals were rotated about a vertical axis with the left ear down in steps of velocity from 30 to 90°/s in 15°/s increments (accelerations >200°/s2). Postflight data were taken one day after flight for 7906 and 3 days after flight for 6151. Before flight, the upward VOR (PreUP) gain was higher, and the gain dropped after flight (PostUp). The downward VOR had a lower gain before flight (PreDown) that was increased after flight (PostDown). Accordingly, the rather striking preflight Up/Down asymmetry of the vertical VOR was decreased after space flight. B, C, Gains of the roll VOR induced by velocity steps between 30 and 90°/s (B), and by sinusoidal oscillation at frequencies between 0.02–0.13 Hz (C). Animals were rotated about a vertical axis in the prone position. Means for preflight testing (± 2 SD) are shown by the heavy solid lines (PRE-MEAN). There was a decrease in roll VOR gains for both 6151 (open symbols) and 7906 (filled symbols) after flight. The decrease was greater for 7906 (50%; filled symbols) than for 6151; open symbols).

By 7 days after landing, the upward aVOR gains had begun to return to preflight levels, and there was no significant difference between pre- and postflight values in both monkeys. The downward aVOR gain dropped to its original level in 6151, but not in 7906. There was no difference in the pitch aVOR gain before and after flight if gains for upward slow phases and downward slow phases were averaged. The pitch aVOR was also measured by rotating the animals sinusoidally at 0.1 Hz, peak velocity 60°/s, about an interaural horizontal axis. This stimulus activates both the vertical canals and the otolith organs. The vertical gain was slightly reduced after landing (6% for 7906 and 9% for 6151), and there was a reduction in the offset of mean velocity in the upward direction that had been present before flight. By the 11th day, the vertical gains had returned so that they were the same or slightly less than the preflight levels for both monkeys. Thus, there was a slight reduction in the gains of the vertical aVOR with otolith activation measured with sinusoids 1–3 days after landing, which had largely returned to the preflight level by the 11th day after recovery. Since the overall vertical gains that were the averages of the up- and down-responses, measured with steps, were unaffected by spaceflight, it is likely that the difference noted in the sinusoidal analysis was due to a change in the otolith contribution to the reflex.

The postflight upward and downward time constants in 782 were 21.3 ± 2.9 s and 10.1 ± 2.4 s, respectively, in response to rotation about a vertical axis while lying on their sides. This is consistent with the vertical time constants in other normal monkeys (Matsuo et al., 1979; Matsuo and Cohen, 1984). Thus, the postflight change in vertical spontaneous nystagmus was not reflected in a change in the dominant time constants of the vertical aVOR.

The roll aVOR was measured in two experimental paradigms: Velocity steps were given with the monkeys in a prone position by rotating them about a vertical naso-occipital axis (Fig. 11B), and the monkeys were sinusoidally oscillated about a horizontal axis while upright (Fig. 11C). Both induce torsional nystagmus, but the first paradigm elicits pure activation of the vertical canals, whereas the second activates both the vertical canals and the otolith organs. The gain of the roll aVOR was reduced in both modes of stimulation, on average by 50% in 7906 and by 15% in 6151 (Fig. 11B, C). This implies that there had been adaptation in central pathways for torsion for activity originating in both the vertical canals and otolith organs during flight, as in humans during 1992 MIR mission (Clarke et al., 1993, 2000).

Spontaneous vertical nystagmus

There was upward spontaneous nystagmus of about 5°/s in both monkeys before the second Cosmos flight, which is common in normal rhesus monkeys. This spontaneous nystagmus was reduced when the animals were first tested, three days after reentry.

High frequency linear vestibulo-ocular reflex

During interaural translation (5 Hz, 0.5 g) postflight, 7906 had an approximate 2/3 reduction in the slope of the function relating lVOR sensitivity to vergence after flight that had not recovered by 16 h after recovery (R+16 h; Figs. 12, 13A). Under the same conditions, 6151 had almost identical responses pre- and postflight (not shown). During dorsoventral translation (5 Hz, 0.5 g) 7906 had from 35–60% reduction in the slope of the function relating the vertical lVOR sensitivity to vergence that had not recovered by R+16 h (Fig. 13B). Under the same conditions, 6151 had responses immediately postflight that were almost identical to the preflight values. Pre- and postflight responses during naso-occipital motion were similar to one another for 6151, but the responses of 7906 were smaller and more variable postflight. This was also the case for motion along oblique axes between naso-occipital and dorsoventral.

Fig. 12.

Fig. 12.

Five-second sample of 5 Hz, 0.5 g peak inter-aural oscillation (ACC) in monkey 6151. In the first traces, ACC is the oscillation of the sled, and HE 1 & HE 2 are right and left horizontal eye position, respectively. In the center traces, HE 1 VSM and VE 1 VSM are right eye horizontal and vertical eye velocity. In the third trace, TE 1 and TE 1 VSM are torsional eye position and eye velocity and VER is vergence position. Note that when vergence was larger, at the left side of the third trace, the oscillations in horizontal eye velocity (large sinusoidal oscillations, middle traces) were larger than when vergence decreased toward the right side of the recording. Vergence had no effect on vertical eye velocity (middle traces). There was a small effect of vergence on torsional eye velocity (third traces).

Fig. 13.

Fig. 13.

A, Changes in sensitivity (degrees of eye movement/cm of oscillation of the linear sled) in horizontal (top clouds) and torsional eye velocity (bottom clouds) after 2229 flight in monkey 7906. VSL VOR represents trials in a stationary lighted surround, while LVOR were trials in darkness. In each graph, A is the intercept, M, the slope and R, the correlation coefficient of the linear fit. The increases in horizontal eye velocity remained linear after flight, but there were significant decreases in the sensitivity (slope) of the responses. Roll responses were relatively small and did not depend on vergence. B, Similar sensitivities for vertical (top clouds) and horizontal eye velocities (bottom clouds) to dorsoventral oscillation with the animal prone. The linear relationship between vergence and vertical eye velocity sensitivity was similar to that for horizontal eye velocity and vergence during interaural acceleration (A), and there was a similar decline in the sensitivity of this relationship after flight that remained for 16 days after landing. Horizontal sensitivity to dorsoventral acceleration was small in all instances.

Low frequency lVOR – off-vertical axis rotation (OVAR)

In preflight testing, steady state eye velocity during OVAR increased as a function of stimulus velocity and of tilt angle for the eight control monkeys, saturating at about 45°/s (Fig. 14A). Steady state horizontal eye velocities induced by OVAR were the same after flight in the monkeys from both the 2044 flight and from the 2229 flight (Fig. 14B), and the phases of the modulations in horizontal slow phase eye velocity were also approximately the same before and after flight. There was an approximate doubling of the amplitude of modulation of horizontal slow phase velocity after the first flight, but not after the second flight. Thus, the animals appeared to be able to sense gravity through the otolith system normally after space-flight and to generate the same steady state level of horizontal slow phase eye velocity after, as before, flight. This implies that the neural mechanism for generating horizontal eye movements had not been substantially altered by adaptation to microgravity.

Fig. 14.

Fig. 14.

A, B, Nystagmus induced by off-vertical axis rotation (OVAR) in darkness at 60°/s about tilted axes before (A) and after (B) COSMOS 2229 space flight for monkey 6151. In both A and B the axis of rotation (A, top trace) was tilted from 0-90° in the dark in 15° increments inducing OVAR nystagmus. The position of the animal about the yaw axis, recorded with a potentiometer that reset each 360°, is shown in the second trace (YAW POS). Upward spontaneous nystagmus was reduced after flight (VER VEL). The amplitude of the horizontal slow phase velocity (HOR VEL) was unchanged after flight, but the modulation in slow phase velocity before flight was increased. There was a prominent modulation in roll eye position (ROLL POS) before flight in response to the lateral tilts during OVAR (A, 3rd trace). After flight the modulation in roll position was decreased (B, 1st trace). C, D, Ocular Counter-Roll (OCR) induced during OVAR by tilts of the axis of rotation from 15 to 90° in 6151 (C) and 7906 (D), before (PRE-MEAN) and after flight (days 1, 7, 11). E, Comparison of postflight OCR in the two flight monkeys and six control monkeys and in the two flight monkeys. As above, PRE-MEAN is the mean of the tests before flight; D1–D11 indicate the tests done on recovery days 1 to 11. The OCR of 6151 and 7906 fell more than 2 D from the preflight means.

Ocular counter-rolling

In microgravity, there is no otolith-induced compensatory torsion of the eyes (ocular counter-rolling, OCR) in response to sustained head on body tilt (Clarke et al., 1993, 2000). OCR, elicited by linear acceleration along the interaural axis and measured by an after-image method, was reduced in two cosmonauts for up to 14 days after landing (Yakovleva et al., 1982), and recovered only at the next test point of 36 days. There was also anti-compensatory torsion (“paradoxical counter-rolling”) in the direction of head tilt in some subjects after long-duration missions (Clarke et al., 2000). In the Spacelab-1 Mission, OCR was measured in four subjects using a photographic technique (Young et al., 1981). Expressed as a gain ratio, OCR in humans was reduced to one side by 28 to 56% one day after landing. OCR, measured by an after-image technique was reduced by 57% for five days in one astronaut after the 1992 Russian–German MIR Space Mission (Hofstetter-Degen et al., 1993). The extensive literature is reviewed in Dai et al., 1994; Clarke et al., 2000; Moore et al., 2001. Thus, there has been fragmentary evidence to indicate that there may be a reduction in the magnitude of OCR. On the other hand, there was no change in OCR in astronauts who flew in the 1998 Neurolab Mission (STS-90) (Moore et al., 2001). The results, however, were quite different for the monkeys that flew on Cosmos 2229.

Dynamic OCR was assessed using OVAR. The OCR elicited by OVAR before and after space flight is shown in Fig. 14A (3rd trace) and Fig. 14B (1st trace). In both instances, OCR was induced by the response to a projection of the gravity vector that rotated relative to the head along the coronal plane. The maximum torsion was induced during OVAR when the gravity vector was aligned with the interaural axis. Responses of monkeys 6151 and 7906 before and after flight for all angles of tilt of the axis of rotation are summarized in Figs. 14C, D. After flight, the mean magnitude of OCR in the flight monkeys was 2.2±0.7° for tilt angles between 60 and 90°. This can be contrasted to the 6.3±0.7° of ocular torsion when the axis of rotation was tilted 60 to 90° in the control monkeys. The mean reduction in dynamic OCR after flight was about 70%. The postflight OCR of the two flight monkeys fell more than two standard deviations below their own preflight means (Fig. 14C, D) and below that of five monkeys from the control group (Fig. 14E). Static OCR was 6.0 ± 0.9° for tilts of 90° in five monkeys tested before flight and in three control monkeys tested in the postflight period.

After space flight, the magnitude of static OCR was reduced in the two flight monkeys to a mean of 1.8 ± 0.7°, a reduction of about 70%. The differences between preflight and postflight OCR, elicited by OVAR, which can also be seen in Fig. 14A, B (ROLL POS, bottom traces), remained over the 11 days of postflight testing and were significant in both flight animals (p ⪡ 0.001). In contrast, there was no change in the OCR of three control monkeys tested before and after flight. These data indicate that there had been long-lasting suppression of OCR after adaptation to microgravity.

Vergence

Vergence has been elicited by naso-occipital linear acceleration on a sled in both frontal and lateral eyed mammals, including humans (Paige, 1991; Paige et al., 1998). Vergence increases when monkeys or humans are linearly accelerated forward at sinusoidal frequencies between 1 and 5 Hz, presumably, serving to help fixate near targets. At low frequencies, the gain of vergence and of other components of the lVOR drop significantly, but considerable vergence would still be expected in response to large linear accelerations during orienting responses. During off-vertical axis rotation (OVAR), the linear acceleration of gravity acts along all head axes in a sinusoidal fashion. For OVAR stimulus velocities of 60°/s with the axis of rotation tilted 90°, there would be sinusoidal linear acceleration of ± 1 g at a frequency of 0.17 Hz. Along the naso-occipital axis, the maximal linear acceleration would be forward when the head is nose-up, similar to that at the onset of forward movement on a linear sled, and backward in the nose-down position. During OVAR, there was not only a continuous and systematic modulation in horizontal, vertical and torsional eye position, but the eyes also converged during each cycle of rotation (Dai et al., 1996). Peak vergence (Fig. 15A, LT-RT POS, third trace) developed when the animal was in the nose-up position. Concurrently, the eyes moved down (VERT POS, fourth trace). When the animal was nose-down, vergence was minimal, and the eyes were elevated. The modulation of vergence and vertical movements of the eyes was 90° out of phase with modulations in torsional eye position, which were maximal in side-down positions.

Fig. 15.

Fig. 15.

A, B Comparison of modulation in vergence induced by OVAR in flight monkey 7906 in preflight and postflight tests from the Cosmos 2229 flight. From top to bottom the traces are right and left eye horizontal position (RIGHT POS, LEFT POS), vergence (LT-RT POS) and vertical eye position (VERT POS). Rotation positions about the animal’s yaw axis is shown under the 4th trace in B and was the same for A. Modulation of vergence was reduced after space flight, but the phase of peak vergence relative to the nose-up position was unaltered. Although there was less vertical nystagmus after flight, the magnitude of modulation of vertical eye position was essentially the same after as before flight. C, Summary of the amplitude of ocular vergence modulation before space flight. Shown are means ±1 SD and a sinusoidal fit (dashed line) of the data of 10 monkeys, including 6151 and 7906 before flight. D, preflight vergence (open symbols) and postflight vergence (solid symbols) for 6151 (circles) and 7906 (squares). The sine fit of the preflight data (dashed line) can be compared to the sine fit of the postflight data (solid line). There was a significant decrease in the postflight vergence for both monkeys.

Mean values of the peak-to-peak amplitude of modulation in vergence as a function of OVAR tilt angle for 10 monkeys and their associated standard deviations are shown in Fig. 15C. They were well approximated by a sinusoid (dashed line), indicating that there was a linear relationship between the amount of OCR and the angle of tilt. When the axis of rotation was tilted 90°, the maximal amplitude of modulation in vergence in these monkeys was 7.8°, and the minimum was 3.2°. The mean modulation of the peak-to-peak amplitude of vergence for all 10 animals at a 90° OVAR tilt angle was 5.5 ± 1.3°. Because the peak GIA occurred in the nose-up position, phases of peak vergence were determined relative to a nose-up position during OVAR. All animals had peak vergence when their heads were rotated close to the nose-up position. The mean phase was −0.9 ± 26.6°. This supports the contention that the naso-occipital acceleration was the factor responsible for the vergence.

After space flight, the modulation in vergence was strikingly reduced in the two flight monkeys. Eye position data from the preflight and first postflight test for 7906 (Fig. 15B), demonstrates the reduction in the amplitude of vergence (LT-RTPOS). The magnitude of vertical eye modulation, which accompanies vergence during naso-occipital linear acceleration (VERT POS), was virtually the same before and after flight. Spontaneous vertical nystagmus was reduced during OVAR after space flight, and the beats of nystagmus were replaced by saccades (Fig. 15B, 4th trace). There was also a reduction in the nystagmus frequency in 7906 that was not found in 6151 or in the previous monkeys after recovery.

Results of postflight testing are summarized in Fig. 15D. As before flight, the data were fit by a sinusoid (Fig. 15D, solid line). Vergence fell at every tilt angle at which a modulation was measurable after flight, with peak vergence being reduced by over 50%. These reductions in modulation of vergence were significant. Test values throughout the postflight period were similar to those on postflight day 1. On postflight day 11, the peak modulation in vergence for 7906 was 1.8° with a phase of 16° with respect to the nose-up position for an OVAR tilt angle of 90°. Under the same condition, the vergence modulation for 6151 was 2.2° with a phase of 6.3°. By contrast, there was neither reduction in vergence modulation nor a significant phase change in two control monkeys that were available for testing in the postflight period.

Spatial orientation of velocity storage

Eye velocity during per- and postrotatory nystagmus, optokinetic nystagmus (OKN) and optokinetic after-nystagmus (OKAN) and the nystagmus induced by centrifugation tends to align with the direction of gravitoinertial acceleration (GIA) (Dai et al., 1991; Wearne et al., 1999; Moore et al., 2004). A similar tendency has also been demonstrated during rapid reorientation of the head during postrotatory nystagmus and OKAN (Dai et al., 1992; Fetter et al., 1996). The process of alignment has three components: (1) The horizontal time constant is reduced according to the projection of the GIA onto the head yaw axis; (2) The vertical and/or roll time constants are increased according to the projection of the GIA onto the head vertical or roll axes; and (3) Vertical and/or torsional cross-coupled components appear, which are not aligned with the angular stimulus vector when the stimulus is given about the yaw axis. Optimally, the amount of axis shift can be assessed during OKAN, recorded in three dimensions with the head in tilted positions, or from vestibular nystagmus during centrifugation when the gravito-inertial acceleration vector is tilted with regard to the head and body, but there are also manifestations of the orientation of eye velocity to the GIA during OKN (Moore et al., 2004). Partial testing can be used to characterize the spatial orientation of the aVOR, specifically, the rapid reduction in yaw eye velocity during postrotatory nystagmus (tilt-dumping) (Waespe et al., 1985). On Earth, this results in a shorter horizontal aVOR time constant than in upright position. If the horizontal aVOR time constant were not to respond to head tilt with regard to gravity after space flight, it would indicate a reduction in sensitivity to spatial orientation of the aVOR.

Evidence for a change in spatial orientation of velocity storage came from two animals that were tested shortly after return from microgravity, one from Cosmos 2044 and the second from Cosmos 2229. Monkey 782 lost the ability to shorten its horizontal time constant when tilted with regard to gravity after the Cosmos 2044 flight (Fig. 15B). During postrotatory nystagmus, the animal was tilted 50° at the upward arrow. Time constants measured from the onset of tilt or at a comparable time 10 s after the onset of the postrotatory nystagmus were 6.7 s after tilt as against 28 s without tilt (Fig. 16A). After flight, there was no effect of tilt on postrotatory nystagmus in this monkey (Fig. 16B), and the time constant of each response, was the same as when it was upright in darkness during perrotatory nystagmus (19.3 ± 1.8 s (n=6) vs 22.1 ± 8.9 s (n=6). Findings were the same 2 and 4 days after landing in this monkey. Control time constants were 17.6 s (± 2.3, n=10) vs tilt time constants of 16.6 s (± 3.0, n=7) on these days. This indicates that the loss of the ability to dump stored slow phase eye velocity persisted for several days after landing in this monkey. This deficit was not present in the second monkey from the same flight, however.

Fig. 16.

Fig. 16.

A, B, Slow phase velocity of per- and postrotatory nystagmus induced by steps of velocity in darkness in monkey 782 before (A) and after (B) the Cosmos 2044 flight. In each set, the animal was rotated in darkness about a vertical axis, inducing per- and postrotatory nystagmus. After the eye velocity had declined to zero, the animal was stopped and 10 s later it was tilted 50° (TILT POS). Before flight (A), this maneuver caused a prompt decline in slow phase velocity. After flight (B), the tilt did not shorten the time course of decline in slow phase velocity. Per- and postrotatory time constants are shown below each response. C–F, Optokinetic nystagmus (OKN), optokinetic after nystagmus (OKAN) and trajectory of axis of eye velocity in horizontal and vertical dimensions on the right. C, D, Horizontal OKN and OKAN were induced with a normal monkey was upright. After the lights were extinguished, OKAN was horizontal and decayed to zero with its characteristic time course. D, The points in the phase plane plots start at the onset of OKAN, which are farthest from the origin, and proceed beat by beat toward the origin where the velocity was again zero. With the animal upright, the eye velocity vector was aligned with both the animal’s yaw axis and the spatial vertical. E, F, When the animal was tilted on its side and given the same stimulus as in C, the time constant of the horizontal component of OKAN was shorter, and the OKAN had a cross-coupled vertical component, which rose and decayed. F, In the phase plane plot, the trajectory of OKAN was initially along the animal’s yaw axis, but then curved toward the animal’s pitch axis. This brought the eye velocity vector close to the spatial vertical at the end of OKAN.

More complete testing for spatial orientation was performed after the Cosmos 2229 flight. Trajectories of eye velocity during OKAN in a normal monkey, upright and tilted with respect to gravity are shown in Fig. 16AD. The angle of the eye velocity vector should be close to gravity in a phase plane plot at the end of OKAN when eye velocity approaches zero (Dai et al., 1991). Before flight, the axis of eye rotation of 7906 for upward coupling from horizontal OKAN at a 90° tilt angle approached the spatial vertical at an angle of 5° (Fig. 17A). Immediately after the flight at R+22 hours, the eye velocity vector was shifted 28° away from gravity toward a body orientation (Fig. 17B). Seven days later, the orientation of eye velocity had returned closer to gravity (Fig. 17C, 7°). Vectors calculated for OKAN with the animals tilted 30, 60 and 90° showed a similar pattern. That is, the spatial orientation of velocity storage towards gravity was altered after space flight and recovered after 7 days, suggesting that monkey 7906 had shifted the orientation of its eye velocity toward the body in Space. A similar shift in spatial orientation of eye velocity was not found in monkey 6151, but this animal was not tested until the third day, 72 h after recovery, by which time there may have been recovery of this function.

Fig. 17.

Fig. 17.

A–C, Trajectory (phase plane) plots of vertical (ordinate) and horizontal (abscissa) eye velocity during cross-coupling of horizontal OKAN, similar to that shown in Fig. 16 F. The animal (7906) was in a 90° tilted, side-down position, and OKN was induced by yaw axis rotation of the visual surround at 60°/s. OKAN slow phase velocities began in each graph on the right, and the velocities progressed toward zero to the left in a curved fashion. Each circle represents the velocity of one slow phase. The solid curved line represents the fit of the data using a modified Levenberg–Marquardt algorithm. The straight line is the trajectory of the last part of the decaying OKAN, showing the slope of the fitted curve as the data approached zero. A, Before flight, the yaw axis eye velocity vector had an angle of 5° from the vertical. B, Twenty-two hours after flight, the eye velocity vector had shifted toward the body axis and was now 28° from the vertical. C, Seven days later, the eye velocity vector had returned to close to its original position and now was deviated 7° from the vertical. D, Analysis of eye velocity vectors (elgenvectors) obtained during OKAN cross-coupling, before (open circles) and 22 h (filled circles) and 7 days (open square) after flight. Values on the ordinate are deviations from the spatial vertical, which is represented by the horizontal line through zero. The abscissa shows the angle of tilt of the axis of rotation during the OKN and OKAN. Animals were tested at 30, 60 and 90° of tilt. Before flight and 7 days after flight, the eye velocity vectors lay close to the spatial vertical. Twenty two hours after recovery, there was a linear increase in the angle of deviation of the eye velocity vectors, representing deviations of the vectors from the spatial vertical. The deviation was maximal (28°) at 90° of tilt. Adapted from Dai et al., Exp. Brain Res. 102, 45–56, 1994, with permission.

Studies of lateral semicircular canal afferents

Single unit recordings were made from horizontal semicircular canal afferents in four rhesus monkeys within the first 48 h following space flight recovery and for 8–11 days thereafter. Monkeys were exposed to step and sinusoidal rotations about an Earth-vertical (yaw) axis. After Cosmos 2044, the mean gain of 29 afferents in 107 tests was higher for four days and then returned to preflight levels. Figure 18 shows typical units from one of the flight monkeys before and after flight during velocity steps (Fig. 18A), sinusoidal rotation at 0.2 Hz, peak velocity 50°/s (Fig. 18B), sum of sines (Fig. 18C), and tilt (Fig. 18D). Note that the preflight and postflight units were not the same. Therefore, differences in resting discharge were not directly comparable. With this caveat, the modulation in responses to step and sine angular accelerations were substantially larger after flight (Fig. 18AC).

Fig. 18.

Fig. 18.

Stimulus traces (left) and time histograms of typical responses of horizontal (lateral) semicircular canal afferents from Cosmos 2044, preflight and on postflight day 1. A, Rotation at 50°/s for 30 s. B, Sinusoidal rotation at 0.2 Hz, 50° peak velocity. C, Rotation with sum of sines. D, 20° tilt forward and back of the animal’s yaw axis. Adapted from Correia et al., J. Appl. Physiol., 1992, Aug. 73 (2 Suppl.): 1125–1265, with permission.

The canal afferents had no response to tilt either before or after flight (Fig. 8D). This experiment was repeated after the Cosmos 2229 flight. On postflight day 1, mean gains from 12 afferents were lower than the mean of 24 afferents before flight (p<0.001), and this difference persisted for 11 days postflight. Correia et al. note: “It is not clear why postflight recordings made from afferents following one flight (COSMOS 2044) showed mean parameters indicating an increase in gain and neural adaptation while the mean postflight recordings made from a second flight (COSMOS 2229) show mean parameters indicating a decrease in gain and no change in neural adaptation. But for both flights, the horizontal semicircular canals were statistically significantly different from those of preflight and synchronous controls. These differences were present while concurrent tests of the horizonal VOR, using the same step paradigms, revealed no differences in slow phase eye velocity between control animals and those that flew in Space. These results suggest that compensation for the altered input from the vestibular sensory receptor (the semicircular canal) probably occurred within the CNS vestibular pathways.”

Discussion

These results show that exposure to microgravity resulted in changes in the linear VOR, the angular VOR, and in the spatial orientation of slow phase velocity produced by the velocity storage component of the angular VOR. The gain of compensatory ocular movements produced by the high frequency sinusoidal oscillation was reduced in one monkey, and the gains of ocular counter-rolling (OCR) and vergence produced by low frequency, interaural and naso-occipital linear acceleration were also substantially lower in 2 monkeys after than before flight. Associated with this, there was a reversal of the asymmetry in vertical nystagmus, and a reduction in the gain of the roll aVOR. Finally, in the monkey that had the largest reduction in response to linear acceleration (7906), the orientation of slow phase eye velocity during OKAN and vestibular nystagmus shifted from a spatial toward a body axis. In contrast, high frequency, horizontal and vertical canal-related responses, generated by angular acceleration in a head coordinate frame of reference, were unaffected by microgravity in post-flight testing. Since the vertical canals had a normal gain after flight when tested with rotation in pitch, it is not likely that a change in the afferent input from the vertical canals was the cause for the reduction in the roll aVOR gain. Rather, there must have been changes in excitability in central pathways for torsion. The adaptive changes in otolith reflexes, in the roll aVOR and in the spatial orientation of eye velocity in the aVOR are likely to contribute to postural, locomotor and gaze instability on reentry after space flight.

The data in these experiments were taken from monkeys whose bodies were restrained. Therefore, these monkeys had only a very limited exposure to linear acceleration during flight. In Space, the otoliths are not activated by static lateral head tilt, and neck receptors do not contribute to OCR (Clarke et al., 1993). Moreover, lateral translations, which are associated with OCR on Earth, mainly induce a horizontal component in Space (Clarke et al., 2000). The relative absence of exposure to linear acceleration, therefore, could have been the cause for the reduction in the ocular/spatial reactions to linear acceleration upon return to Earth. Lateral translation when turning corners was also absent in Space, which might explain the 15–50% reduction in gain of the roll aVOR.

Of interest in this regard are recent results from the NASA Neurolab Mission (STS-90), which demonstrated that these otolith-ocular orienting responses were well maintained during space flight (Clément et al., 2001; Moore et al., 2001, 2004). It is possible that this difference in response to microgravity between the monkeys in the COSMOS flights and the astronauts in the Neurolab Mission was due to a species difference. More likely, however, is that the preservation of the otolith-ocular orienting and compensatory reflexes was due to the active movement and frequent centrifugation experienced by the astronauts in Space on STS-90. If this is correct, then a valuable lesson has come from the monkey experiments. Namely, that a program of active head movement with exposure to linear acceleration is an appropriate countermeasure for the reduction in the gain of OCR, vergence and the roll aVOR. Such a countermeasure could also help maintain the gain of vestibulo-sympathetic reflexes, which serve as a first line of defense in maintaining blood pressure upon standing (Kaufmann et al., 2002). A drop in the gain of such reflexes could contribute to the orthostatic hypotension that commonly follows space flight. Thus, the data in these monkeys suggest that the gain of roll and vergence may be much more malleable than has commonly been assumed. Unfortunately, the only way to test this would be in Space, where there is a prolonged absence of gravity, and the opportunities for such experiments are few.

Our results also show that there is considerable variation between individuals exposed to essentially similar conditions in Space. Microgravity was associated with a striking reduction in the high frequency lVOR gain in 7906, whereas the compensatory lVOR was essentially normal in 6151, although 6151 was not tested until the third day after recovery. This mirrors similar variability in humans exposed to microgravity. On the other hand, there was a striking similarity in the increased sensitivity of the aVOR during active head turns, in the saccadic hypermetria during lateral gaze shirts, and in the increase in the sensitivity of units in MVN and flocculus to head turns in some of these same monkeys. Afferent activity from the lateral semicircular canals also varied considerably between Cosmos flights 2044 and 2229 (Correia et al., 1992; Correia, 1998) in some of these same monkeys, although the passive aVOR gains were unaffected (Cohen et al., 1992; Dai et al., 1994). Some of these changes may have been a consequence of the behavioral state or the experimental conditions, interacting with exposure to microgravity, but there also seems to be an individual difference of response to essentially similar conditions.

Eye velocity during nystagmus due to excitation of the slow component of the aVOR tends to align with the spatial vertical when the head is tilted with regard to the GIA (Dai et al., 1991, 1992). In both flights, this spatial orientation was affected in one of the two monkeys available for testing shortly after landing. The shift in orientation disappeared over a time course of several days after reentry into a gravitational environment (Cohen et al., 1992; Dai et al., 1994). The reduction in the direct orienting response of OCR and vergence persisted for a longer period than the indirect orienting response of OKAN cross-coupling, which is produced through a different mechanism, i.e., through velocity storage. An important aspect of re-adaptation upon the reentry is to reorient to gravity so that the body posture is maintained during motion. This may explain why the reorientation of velocity storage, as reflected in OKAN cross-coupling, occurred sooner than the recovery of other ocular orienting reactions produced by the lVOR.

In this chapter, we have summarized experiments that provide a consolidated body of new data that demonstrate changes that can be expected in the vestibulo-ocular reflex and the central vestibular system after space flight. The experiments in Sections 2 and 3 also show the unique value of the monkey as a model for studying effects of human vestibular adaptation in Space, wherein behavior and single unit recordings can be combined in a single animal that has many similarities to humans. It is hoped that the work described in this chapter will aid in understanding the complex phenomena that accompany adaptation to microgravity, especially in relation to long-duration space flight. There is a larger reason to promote the use of experimental animals in Space. There is no other way to understand the critical role of gravity on the formation and structure of the nervous system. Consequently, an essential component of future space-related experiments should be directed toward determining how afferent input from the otoliths and semicircular canals is altered and how central processing is changed in microgravity in experimental animals.

Acknowledgment

We thank Jun Maruta for assistance. This work was supported by NASA Grants NAG 2-573 (BC), NAG 2-703 (BC), NASA Contract NAS 9-19441(BC), NCC2-1173 (GRH), NAG 2-946 (GRH), NIH Grants: DC02451 (GRH), DC04996 (SY), DC05204, and EY01867.

Footnotes

1

The vertical canals contribute to the neural response to head movement in the yaw plane. Therefore, vertical canal-related units would also be modulated with this stimulus, and it is possible that some of the activated neurons were actually more closely related to the vertical canals. Activity of the unit shown in Fig. 4 was modulated during horizontal but not vertical eye movements, and it is likely that this unit was a lateral canal-related neuron.

2

The acceleration in the preflight testing was higher during the rapid drop than inflight because gravity added a downward pull to that provided by the spring mechanism (see Methods). As described in Methods, the linear acceleration was only significantly above threshold for detection during the rapid drop in Phase 3 and the stop-reaction in Phase 4.

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