Twofold effect of blue light on a circadian rhythm in Acetabularia

Abstract

The circadian chloroplast migration in Acetabularia mediterranea was monitored by continuously measuring the transmission of the cells near the apex. Under continuous red light the amplitude of the rhythm decreased rapidly within a few days. However, circadian changes of chloroplast density were still detectable even after 28 days of red light, indicating the persistence of the rhythm. When blue light was added after red light preirradiation of several days phase shifts were observed which were expressed as advances as well as delays. The period of the rhythm proved to be strongly dependent on the intensity of the continuous blue light which was given in addition to red light. Different red light intensities did not change the period. The occurrence of both effects indicates that the sensory transduction of blue light photoreception in Acetabularia works in two different ways: quanta counting processes and processes of light intensity measurement.     

The Polar Organization of the Growing Chara Rhizoid and the Transport of Statoliths are Actin-Dependent*

Horizontally positioned Chara rhizoids continue growth without gravitropic bending when the statoliths are removed from the apex by basipetal centrifugation. The transport of statoliths in centrifuged rhizoids is bidirectional: 50–60 % of the statoliths are re-transported on a straight course to the apex at velocities from 1 to 14 μm . min^?1 increasing towards the rhizoid tip. The centrifuged statoliths which are located closest to the nucleus are basipetally transported and caught up in the cytoplasmic streaming of the cell. Those statoliths which are located near the apical side of the nucleus are transported either apically or basally. A de-novo-formation of statoliths was not observed. After retransport to the apex some statoliths transiently sediment, a process which can induce a local inhibition of cell wall growth. The rhizoid bends again gravitropically only if a few statoliths finally sediment in the apex; the more statoliths that sediment in the apex the shorter the radius of bending becomes. The transport of statoliths is mediated by actin filaments which form a network of thin filaments in the apical and subapical zone of the rhizoid, and thicker parallel bundles in the basal zone where cytoplasmic streaming occurs. Both subpopulations of actin filaments overlap in the nucleus zone.     

Micromanipulation of statoliths in gravity-sensing Chara rhizoids by optical tweezers

Infrared laser traps (optical tweezers) were used to micromanipulate statoliths in gravity-sensing rhizoids of the green alga Chara vulgaris Vail. We were able to hold and move statoliths with high accuracy and to observe directly the effects of statolith position on cell growth in horizontally positioned rhizoids. The first step in gravitropism, namely the physical action of gravity on statoliths, can be simulated by optical tweezers. The direct laser microirradiation of the rhizoid apex did not cause any visible damage to the cells. Through lateral positioning of statoliths a differential growth of the opposite flank of the cell wall could be induced, corresponding to bending growth in gravitropism. The acropetal displacement of the statolith complex into the extreme apex of the rhizoid caused a temporary decrease in cell growth rate. The rhizoids regained normal growth after remigration of the statoliths to their initial position 10–30 m basal to the rhizoid apex. During basipetal displacement of statoliths, cell growth continued and the statoliths remigrated towards the rhizoid tip after release from the optical trap. The resistance to statolith displacement increased towards the nucleus. The basipetal displacement of the whole complex of statoliths for a long distance (>100 m) caused an increase in cell diameter and a subsequent regaining of normal growth after the statoliths reappeared in the rhizoid apex. We conclude that the statolith displacement interferes with the mechanism of tip growth, i.e. with the transport of Golgi vesicles, either directly by mechanically blocking their flow and/or, indirectly, by disturbing the actomyosin system. In the presence of the actin inhibitor cytochalasin B the optical forces required for acropetal and basipetal displacement of statoliths were significantly reduced to a similar level. The lateral displacement of statoliths was not changed by cytochalasin B. The results indicate: (i) the viscous resistance to optical displacement of statoliths depends mainly on actin, (ii) the lateral displacement of statoliths is not impeded by actin filaments, (iii) the axially directed actin-mediated forces against optical displacement of statoliths (for a distance of 10 m) are stronger in the basipetal than in the acropetal direction, (iv) the forces acting on single statoliths by axially oriented actin filaments are estimated to be in the range of 11–110 pN for acropetal and of 18–180 pN for basipetal statolith displacements.Abbreviation CB cytochalasin B This work was supported by the Bundesminister für Forschung und Technologie, and by Fonds der Chemischen Industrie. We thank Professor Dr. A. Sievers (Botanisches Institut, Universität Bonn, Germany) for helpful discussions.     

Morphogenesis of the fern protonema

Summary At the apex of the protonema ofDryopteris varia, a club-shaped papilla is differentiated after the protonema was segmented into six or seven cells in the normal development. If the sporeling is reared in medium containing IAA, formation of the apical papilla is much accelerated to take place at two- or three-cell stage when the concentration of IAA is 1 to 0.01 ppm. But if it is reared in a medium of a higher concentration of IAA, 10 to 100 ppm, the same apex differentiates a rhizoid. That is to say, it depends upon quantitative relations of auxin as to whether the apex of protonema forms a papilla or a rhizoid. With 3 Figures     

Screening pigment,aperture and sensitivity in the dung beetle superposition eye

Summary Sensitivity to light was investigated in the refracting superposition eye of the dung beetle Onitis alexis using electrophysiological measurements and optical modelling. Intracellular recordings were made from single retinula cells over 24-h periods, with cells light and dark adapted, in order to measure the response/intensity (V-LogI) functions. The combined effects of a circadian rhythm and light adaptation allow the determination of the relative contributions of screening-pigment migration and transduction gain to changes in sensitivity in the eye. Between the extremes of dark adaptation at night and light adaptation during the day, the maximum sensitivity change possible is at least 4 log units, of which approximately 2 log units can be accounted for by changes in the transduction gain and at least 2 log units by screening-pigment migration. The role of the superposition aperture (the number of facets that contribute light to one rhabdom) in 3 species of dung beetle was investigated with an optical ray-tracing model of the eye. The facets of the superposition aperture do not contribute light equally to the target rhabdom; except in one species, the greatest contribution comes from facets located away from both the centre and periphery of the aperture. Light adaptation increases the optical density of the superposition aperture and decreases its size.     

Phase resetting of the circadian rhythm of carbon dioxide assimilation inBryophyllum leaves in relation to their malate content following brief exposure to high and low temperatures,darkness and 5% carbon dioxide

Leaves ofBryophyllum fedtschenkoi show a persistent circadian rhythm in CO₂ assimilation when kept in continuous illumination and normal air at 15°C. The induction of phase shifts in this rhythm by exposing the leaves for four hours at different times in the circadian cycle to 40° C, 2° C, darkness and 5% CO₂ have been investigated. Exposure to high temperature has no effect on the phase at the apex of the peak but is effective at all other times in the cycle, whereas exposure to low temperature, darkness or 5% CO₂ is without effect between the peaks and induces a phase shift at all other times. The next peak of the rhythm occurs 17 h after a 40° C treatment and 7–10 h after a 2° C, dark or 5% CO₂ treatment regardless of their position in the cycle. When these treatments are given at times in the cycle when they induce maximum phase shifts, they cause no change in the gross malate status of the leaf. The gross malate content of the leaf in continuous light and normal air at 15% shows a heavily damped circadian oscillation which virtually disappears by the time of the third cycle, but the CO₂ assimilation rhythm persists for many days. The generation of the rhythm, and the control of its phase by environmental factors are discussed in terms of mechanisms that involve the synthesis and metabolism of malate in specific localised pools in the cytoplasm of the leaf cells.     

Circadian Control of Dendrite Morphology in the Visual System of Drosophila melanogaster

Background

In the first optic neuropil (lamina) of the fly''s visual system, monopolar cells L1 and L2 and glia show circadian rhythms in morphological plasticity. They change their size and shape during the day and night. The most pronounced changes have been detected in circadian size of the L2 axons. Looking for a functional significance of the circadian plasticity observed in axons, we examined the morphological plasticity of the L2 dendrites. They extend from axons and harbor postsynaptic sites of tetrad synaptic contacts from the photoreceptor terminals.

Methodology/Principal Findings

The plasticity of L2 dendrites was evaluated by measuring an outline of the L2 dendritic trees. These were from confocal images of cross sections of L2 cells labeled with GFP. They were in wild-type and clock mutant flies held under different light conditions and sacrified at different time points. We found that the L2 dendrites are longest at the beginning of the day in both males and females. This rhythm observed under a day/night regime (LD) was maintained in constant darkness (DD) but not in continuous light (LL). This rhythm was not present in the arrhythmic per⁰¹ mutant in LD or in DD. In the clock photoreceptor cry^b mutant the rhythm was maintained but its pattern was different than that observed in wild-type flies.

Conclusions/Significance

The results obtained showed that the L2 dendrites exhibit circadian structural plasticity. Their morphology is controlled by the per gene-dependent circadian clock. The L2 dendrites are longest at the beginning of the day when the daytime tetrad presynaptic sites are most numerous and L2 axons are swollen. The presence of the rhythm, but with a different pattern in cry^b mutants in LD and DD indicates a new role of cry in the visual system. The new role is in maintaining the circadian pattern of changes of the L2 dendrite length and shape.     

Spatial Organization of Calcium Signaling Involved in Cell Volume Control in the Fucus Rhizoid

Subprotoplasts prepared from different regions of rhizoid and thallus cells of Fucus zygotes displayed mechanosensitive plasma membrane channels in cell-attached patch-clamp experiments by using laser microsurgery. In excised patches, this channel was found to be voltage gated, carrying K+ outward and Ca2+ inward, with a relative permeability of Ca2+/K+ of 0.35 to 0.5, and an increased open probability at membrane potentials more positive than -80 mV. No significant difference was found in the density of this channel type from different regions of rhizoid or thallus cells. Hypoosmotic treatment of intact zygotes induced dramatic transient elevations of cytoplasmic Ca2+, initiating at the rhizoid apex and propagating in a wavelike manner to subapical regions. Localized initiation of the Ca2+ transient correlated with greater osmotic swelling at the rhizoid apex compared with other regions of the zygote. Ca2+ transients exhibited a refractory period between successive hypoosmotic shocks, during which additional transients could not be elicited and the ability to osmoregulate was impaired. Buffering the Ca2+ transients with microinjected Br2BAPTA similarly reduced the ability of rhizoid cells to osmoregulate. Ca2+ influx was associated with the initiation of the Ca2+ transient in apical regions, whereas intracellular sources contributed to its propagation. Thus, localized signal transduction is patterned by interactions of the cell wall, plasma membrane, and intracellular Ca2+ stores.     

Simulated microgravity influences circadian rhythm of NIH3T3 cells

Gravity heavily influences living organisms on earth including their circadian rhythm, which is fundamentally important for coordinately physiology in organisms as diverse as cyanobacteria, fungus and humans. Numerous researches have revealed that microgravity in outer space can affect circadian rhythm of astronauts and rodent animals, but the mechanism remains unknown. Using rotary cell culture system to simulate microgravity environment, we investigated the role of simulated microgravity in regulating the circadian rhythm of NIH3T3 cells. Our experiments found that simulated microgravity can not only influence the mRNA level of some core circadian genes, but also modify the circadian rhythm of Per1 and Per2 synchronized after phorbol myristate acetate treatment. Remarkably, MEK/ERK pathway was transiently activated after a 2-h simulated microgravity treatment, with a significant upregulation of Kras, Raf1 and p-ERK1/ERK2. Moreover, U0126, a selective inhibitor of MEK/ERK pathway, could disrupt the circadian rhythm of Per1 and Per2 synchronized after simulated microgravity treatment. Together, our results unveil that simulated microgravity could act like a zeitgeber to influence the circadian rhythm of NIH3T3 by acting on MEK/ERK pathway, indicating that MEK/ERK pathway may act as a bridge which connects cells mechanotransduction pathway and circadian rhythm regulation.     

On optical receivers in the pathway implicated in regulating the human circadian rhythm

Biological and mathematical grounding was provided for the mechanism that is responsible for the optical radiation-dependent regulation of the human circadian rhythm that involves the well-known retinal photoreceptors, rods and blue-sensitive cones. It was shown that light-sensitive retinal ganglion cells are unable to act as receivers of optical radiation. Two spectral channels involved in regulating the circadian rhythm were observed in the retino-hypothalamic pathway. An analytical expression for the function of the relative spectral circadian efficiency was obtained for Scalculations and mathematical modeling of the human circadian rhythm.

     

Isolation of a cell-fusion hormone from Griffithsia pacifica kylin,a red alga

Filaments of Griffithsia pacifica replace dead cells by the process of cell repair. When an intercalary cell is killed, but its cell wall remains intact holding the two halves of the plant together, the cell above it produces a repair rhizoid cell; the cell below it produces a specialized, rhizoid-like repair shoot cell. The repair rhizoid and shoot grow towards each other, meet, and fuse to form a single shoot cell. Evidence from observations of cell repair in vivo has indicated that the repair rhizoid produces a hormone or hormones which induce the production of the repair shoot, maintain the rhizoid-like morphology and growth of the repair shoot, and attract it to the repair rhizoid for fusion. This hormone has been named rhodomorphin. Using an artificial cell-fusion system we show that repair rhizoids and normal rhizoids, but no shoot cell, can induce decapitated filaments to form repair shoot cells. Decapitated filaments form repair shoot cells only when they are exposed to the hormone within 4–6 h after decapitation; after this time they lose their sensitivity to the hormone. A method has been developed for isolating, and assaying for, the cell-fusion hormone. Rhodomorphin retains its activity for several days at room temperature and for at least two years at-16° C.     

Poly(a)+ rna during vegetative development ofacetabularia peniculus

Summary In the juvenile stage, the diploid giant-celled green algae Acetabularia spp. are differentiated into an upright stalk and an irregularly branched rhizoid. Early amputation and grafting experiments as well as biochemical and molecular analyses have shown that mRNA (as poly(A)⁺ RNA) is continuously supplied from the primary nucleus in the rhizoid and accumulates in the stalk apex. In the present study, localization of poly(A)⁺ RNA in the juvenile stage of theAcetabularia peniculus was investigated by fluorescent in situ hybridization using oligo(dT) as a probe. The signal was localized in the apical cytoplasm and, in addition, multiple longitudinal striations throughout the stalk and rhizoid cytoplasm. A large portion of the poly(A)⁺ RNA striations exhibited structural polarity, broadened at one end and gradually thinned toward the other end. Some of the striations in the rhizoid cytoplasm were continuous with a zone of signal in the area of the perinuclear rim. The poly(A)⁺ RNA striations were associated with thick bands of longitudinal actin bundles which run through the entire length of the stalk. Cytochalasin D caused fragmentation of the actin bundles and irregular distribution of the fluorescent signal. We suggest that the poly(A)⁺ RNA striations constitute a hitherto unknown form of packaged mRNA that is transported over large distances along the actin cytoskeleton to be stored and expressed in the growing apex.     

Vasopressin Antagonist Disrupts the Circadian Rhythm of Water Intake on Suprachiasmatic Injection

The present study makes an attempt to find out the action of arginine vasopressin (AVP) and its antagonist d-(CH₂)₅Tyr (Me) AVP applied at the suprachiasmatic nuclei (SCN) on the circadian rhythm of water intake. Chronic implantation of a 22 G stainless steel cannula for injection was performed using a stereotaxic technique under Nembutal anesthesia. AVP and its antagonist were injected into the SCN of free-moving rats at the beginning of light and dark phases of the light-dark (LD) cycle. Injections of AVP during either phase did not disrupt the circadian pattern of water intake while the injections of the antagonist disrupted it. The findings are suggestive of the involvement of AVP as a mediator of the circadian rhythm of water intake at the level of the neural pacemaker, SCN.     

Locomotor activity rhythm in four wrasse species under varying light conditions

Under controlled laboratory conditions, the locomotor activity rhythms of four species of wrasses (Suezichthys gracilis, Thalassoma cupido, Labroides dimidiatus andCirrhilabrus temminckii) were individually examined using an actograph with infra-red photo-electric switches in a dark room at temperatures of 21.3–24.3°C, for 7 to 14 days. The locomotor activity ofS. gracilis occurred mostly during the light period under a light-dark cycle regimen (LD 12:12; 06:00-18:00 light, 18:00-06:00 dark). The locomotor activity commenced at the beginning of the light period and continued until a little before the beginning of dark period. The diel activity rhythm of this species synchronizes with LD. Under constant illumination (LL) this species shows distinct free-running activity rhythms varying in length from 23 hrs. 39 min. to 23 hrs. 47 min. Therefore,S. gracilis appears to have a circadian rhythm under LL. However, in constant darkness (DD), the activity of this species was greatly suppressed. All the fish showed no activity rhythms in DD conditions. After DD, the fish showed the diel activity rhythm with the resumption of LD, but this activity began shortly after the beginning of light period. The fish required several days to synchronize with the activity in the light period. Therefore,S. gracilis appeared to continue the circadian rhythm under DD. InT. cupido, the locomotor activity commenced somewhat earlier than the beginning of the light period and continued until the beginning of the dark period under LD. The diel activity rhythm of this species synchronizes with LD. Under LL, four of the five specimens of this species tested showed free-running activity rhythms for the first 5 days or longer varying in length from 22 hrs. 54 min. to 23 hrs. 39 min. Although the activity of this species was suppressed under DD, two of five fish showed free-running activity rhythms throughout the experimental period. The lengths of such free-running periods were from 23 hrs. 38 min. to 23 hrs. 50 min. under DD. Therefore, it was ascertained thatT. cupido has a circadian rhythm. InL. dimidiatus, the locomotor activity rhythm under LD resembled that observed inT. cupido. The diel activity rhythm of this species synchronizes with LD. Under LL, four of seven of this species showed free-running activity rhythms throughout the experimental period. The lengths of such free-running periods were from 23 hrs. 07 min. to 25 hrs. 48 min. Although the activity of this species was suppressed under DD, three of five fish showed free-running activity rhythms throughout the experimental period. The lengths of such free-running periods were from 23 hrs. 36 min. to 23 hrs. 41 min. under DD. Therefore, it was ascertained thatL. dimidiatus has a circadian rhythm. Almost all locomotor activity of C.temminckii occurred during the light period under LD. The diel activity rhythm of this species coincides with LD. Under LL, two of four of this species showed free-running activity rhythms throughout the experimental period. The lengths of such free-running periods were from 23 hrs. 32 min. to 23 hrs. 45 min. Although the activity of this species was suppressed under DD, one of the four fish showed free-running activity rhythms throughout the experimental period. The length of the free-running period was 23 hrs. 21 min. under DD. Therefore,C. temminckii appeared to have a circadian rhythm. According to field observations,S. gracilis burrows and lies in the sandy bottom whileT. cupido, L. dimidiatus, andC. temminckii hide and rest in spaces among piles of boulders or in crevices of rocks during the night. It seems that the differences in nocturnal behavior among the four species of wrasses mentioned above are closely related to the intensity of endogenous factors in their locomotor activity rhythms.     

Protoplasts from Phaseolus coccineus L. Pulvinar Motor Cells Show Circadian Volume Oscillations

The circadian movement of the lamina of the primary leaf of Phaseolus coccineus is mediated by circadian volume changes of the extensor and flexor cells in the upper and lower half of the laminar pulvinus. Isolated protoplasts from the extensor, flexor, and flank cells of the pulvinus showed a circadian volume rhythm with a period longer than 24 h. In the case of the flexor protoplasts, we found a period length of 28 h, which is similar to that of the pulvinar cells in situ. In the extensor protoplasts, the volume rhythm was synchronized with 14-h light/10-h dark cycles. The larger volume was correlated with the early hours in the light period and the smaller volume with the dark period, as would be expected from the behavior of the extensor cells in situ.     

Mirror imaging phase response curves obtained for the circadian rhythm of a bat with single steps of light and darkness∗

Abstract

The circadian rhythm in the flight activity of a tropical microchiropteran bat Taphozous melanopogon responds at all phases with delay phase shifts to single light‐on steps (DD/LL transfers). The circadian rhythm responds at all phases with advance phase shifts to single light‐off steps (LL/DD transfers). Phase shifts were measured from the delays or advances of the onsets of flight activity on days following DD/LL and LL/DD transfers relative to the temporal course of the onsets of activity in controls. The magnitude of the phase shifts was a function of the phases in which the transfers were made. The On‐PRC and Off‐PRC plotted from such data are mirror‐images in their time‐course and wave‐form.

The phase shifts of the circadian rhythm in either direction were accompanied by changes in period (for the duration of our recordings after die transfer). The period lengthened following a delay shift and it shortened following an advance shift. The phase shifts are abrupt and discernible in the first cycle after perturbation. There are no transients.     

Correlation between circadian periods and cellular activities in Paramecium bursaria

Paramecium bursaria shows a circadian rhythm of photoaccumulation: photoaccumulation is stronger during the day than at night. We obtained five strains of P. bursaria having different circadian periods under continuous light conditions, ranging from 20.9 to 27.9 h. Various physiological activities were compared in the cells of these strains. The periods of contractile vacuole contraction were in the range 10–15 s, which was almost proportional to the periods of the circadian rhythm in each strain. Swimming velocities were inversely proportional to the circadian period; i.e. swimming velocities were high in strains whose circadian periods were short. Resting membrane potential was more depolarized in strains with longer circadian periods. Finally, the membrane resistance of the resting state was reduced in proportion to the increase of the circadian period. Such correlation between the cellular properties and the circadian period suggests that the circadian clock mechanism is associated with various physiological activities of the cell.     

Control of the circadian rhythm of carbon dioxide assimilation in Bryophyllum leaves by exposure to darkness and high carbon dioxide concentrations

The circadian rhythm of CO₂ assimilation in detached leaves of Bryophyllum fedtschenkoi at 15° C in normal air and continuous illumination is inhibited both by exposure to darkness, and to an atmosphere enriched with 5% CO₂. During such exposures substantial fixation of CO₂ takes place, and the malate concentration in the cell sap increases from about 20 mM to a constant value of 40–50 mM after 16 h. On transferring the darkened leaves to light, and those exposed to 5% CO₂ to normal air, a circadian rhythm of CO₂ assimilation begins again. The phase of this rhythm is determined by the time the transfer is made since the first peak occurs about 24 h afterwards. This finding indicates that the circadian oscillator is driven to, and held at, an identical, fixed phase point in its cycle after 16 h exposure to darkness or to 5% CO₂, and it is from this phase point that oscillation begins after the inhibiting condition is removed. This fixed phase point is characterised by the leaves having acquired a high malate content. The rhythm therefore begins with a period of malate decarboxylation which lasts for about 8 h, during which time the malate content of the leaf cells must be reduced to a value that allows phosphoenolpyruvate carboxylase to become active. Inhibition of the rhythm in darkness, and on exposure to 5% CO₂ in continuous illumination, appears to be due to the presence of a high concentration of CO₂ within the leaf inhibiting malic enzyme which leads to the accumulation of high concentrations of malate in the leaf cells. The malate then allosterically inhibits phosphoenolpyruvate carboxylase upon which the rhythm depends. The results give support to the view that malate synthesis and breakdown form an integral part of the circadian oscillator in this tissue.Abbreviations B. Bryophyllum - PEPCase phosphoenolpyruvate carboxylase     

Evidence for a Plastic Dual Circadian Rhythm in the Oyster Crassostrea gigas

Although a significant body of literature has been devoted to the chronobiology of aquatic animals, how biological rhythms function in molluscan bivalves has been poorly studied. The first objective of this study was to determine whether an endogenous circadian rhythm does exist in the oyster, Crassostrea gigas. The second objective was to characterize it in terms of robustness. To answer these questions, the valve activity of 15 oysters was continuously recorded for 2 mo in the laboratory under different entrainment and free-running regimes using a high-frequency noninvasive valvometer. The present work demonstrates the presence of a circadian rhythm in the oyster Crassostrea gigas. First, oysters were entrained by 12?L:12 D conditions. Then, free-running conditions (D:D and L:L) indicated that the most frequently observed period ranged from 20 to 28?h, the circadian range. That endogenous circadian rhythm was characterized as weak. Indeed, the period (τ) of the individual animals exhibited high plasticity in D:D and L:L, and the animals immediately followed a 4-h phase advance or delay. Additionally, C. gigas appeared as a dual organism: all oysters were nocturnal at the beginning of the laboratory experiment (January), whereas they were diurnal at the end (March). That shift was progressive. Comparison with a full-year in situ record showed the same behavioral duality as observed in the laboratory: the animals were nocturnal in autumn–winter and diurnal in spring–summer. The significant advantage of a plastic and dual circadian rhythm in terms of adaptability in a highly changing environment is discussed. (Author correspondence: d.tran@epoc.u-bordeaux1.fr)