Microgravity tissue engineering

Summary Tissue engineering studies were done using isolated cells, three-dimensional polymer scaffolds, and rotating bioreactors operated under conditions of simulated microgravity. In particular, vessel rotation speed was adjusted such that 10 mm diameter × 2 mm thick cell-polymer constructs were cultivated in a state of continuous free-fall. Feasibility was demonstrated for two different cell types: cartilage and heart. Conditions of simulated microgravity promoted the formation of cartilaginous constructs consisting of round cells, collagen and glycosaminoglycan (GAG), and cardiac tissue constructs consisting of elongated cells that contracted spontaneously and synchronously. Potential advantages of using a simulated microgravity environment for tissue engineering were demonstrated by comparing the compositions of cartilaginous constructs grown under four different in vitro culture conditions: simulated microgravity in rotating bioreactors, solid body rotation in rotating bioreactors, turbulent mixing in spinner flasks, and orbital mixing in petri dishes. Constructs grown in simulated microgravity contained the highest fractions of total regenerated tissue (as a percent of construct dry weight) and of GAG, the component required for cartilage to withstand compressive force.     

Limited transfer of podokinetic after-rotation from kneeling to standing

Following stepping in place on a rotating treadmill, subjects inadvertently rotate when asked to step in place without vision. This response is called podokinetic after-rotation (PKAR). The purpose of this study was to determine whether PKAR transfers across tasks with different lower limb configurations, that is, from kneeling to stepping. We hypothesized that PKAR would transfer from kneeling to stepping for two reasons. First, there have been several demonstrations of robust PKAR transfer from forward to backward walking, stepping to hopping, running to walking, and from one limb to another. Second, we thought that afferent information regarding hip rotation was likely a key source of information to guide podokinetic adaptation and since hip rotation would be preserved in both stimulation conditions we expected to see little difference between the conditions. We compared the PKAR responses recorded in standing from 13 healthy young volunteers after either standard stepping on a rotating treadmill or stepping while kneeling (kneel-stepping) on a rotating treadmill. Subjects performed two sessions of podokinetic (PK) stimulation, one stepping and one kneel-stepping on a rotating treadmill. Following the PK stimulation, subjects were blindfolded and asked to step in place in standing. Angular velocity of trunk rotation during PKAR from the two sessions was calculated and compared. The maximum angular velocities of PKAR recorded in stepping were significantly higher following the stepping session than following the kneel-stepping session (9.10 +/- 8.9 and 2.94 +/- 1.6 deg/s, respectively). This was despite the fact that hip rotation excursion during PK stimulation was significantly greater in kneel-stepping (18.7 +/- 3.6 deg) than in stepping (12.2 +/- 2.6 deg). These results indicate very little transfer from kneeling to stepping and suggest that afferent information regarding hip rotation is not the only or even the major source of limb position sense information used to drive locomotor trajectory adaptation.     

Mechanics of Coriolis stimulus and inducing factors of motion sickness.

To specify inducing factors of motion sickness comprised in Coriolis stimulus, or cross-coupled rotation, the sensation of rotation derived from the semicircular canal system during and after Coriolis stimulus under a variety of stimulus conditions, was estimated by an approach from mechanics with giving minimal hypotheses and simplifications on the semicircular canal system and the sensory nervous system. By solving an equation of motion of the endolymph during Coriolis stimulus, rotating angle of the endolymph was obtained, and the sensation of rotation derived from each semicircular canal was estimated. Then the sensation derived from the whole semicircular canal system was particularly considered in two cases of a single Coriolis stimulus and cyclic Coriolis stimuli. The magnitude and the direction of sensation of rotation were shown to depend on an angular velocity of body rotation and a rotating angle of head movement (amplitude of head oscillation when cyclic Coriolis stimuli) irrespective of initial angle (center angle) of the head relative to the vertical axis. The present mechanical analysis of Coriolis stimulus led a suggestion that the severity of nausea evoked by Coriolis stimulus is proportional to the effective value of the sensation of rotation caused by the Coriolis stimulus.     

Limited transfer of podokinetic after-rotation from kneeling to standing

Following stepping in place on a rotating treadmill, subjects inadvertently rotate when asked to step in place without vision. This response is called podokinetic after-rotation (PKAR). The purpose of this study was to determine whether PKAR transfers across tasks with different lower limb configurations, that is, from kneeling to stepping. We hypothesized that PKAR would transfer from kneeling to stepping for two reasons. First, there have been several demonstrations of robust PKAR transfer from forward to backward walking, stepping to hopping, running to walking, and from one limb to another. Second, we thought that afferent information regarding hip rotation was likely a key source of information to guide podokinetic adaptation and since hip rotation would be preserved in both stimulation conditions we expected to see little difference between the conditions. We compared the PKAR responses recorded in standing from 13 healthy young volunteers after either standard stepping on a rotating treadmill or stepping while kneeling (kneel-stepping) on a rotating treadmill. Subjects performed two sessions of podokinetic (PK) stimulation, one stepping and one kneel-stepping on a rotating treadmill. Following the PK stimulation, subjects were blindfolded and asked to step in place in standing. Angular velocity of trunk rotation during PKAR from the two sessions was calculated and compared. The maximum angular velocities of PKAR recorded in stepping were significantly higher following the stepping session than following the kneel-stepping session (9.10?±?8.9 and 2.94?±?1.6?deg/s, respectively). This was despite the fact that hip rotation excursion during PK stimulation was significantly greater in kneel-stepping (18.7?±?3.6?deg) than in stepping (12.2?±?2.6?deg). These results indicate very little transfer from kneeling to stepping and suggest that afferent information regarding hip rotation is not the only or even the major source of limb position sense information used to drive locomotor trajectory adaptation.     

A computational approach to investigate optimal cutting speed configurations in rotational needle biopsy cutting soft tissue

The rotational cutting method has been used in needle biopsy technologies to sample tough tissues, such as calcifications in the breast. The rotational motion of the needle introduces shear forces to the cutting surface such that the cutting force in the axial direction is reduced. As a result, tissue samples with large volume and better quality can be obtained. In order to comprehensively understand the effect of the needle rotation to the axial cutting force under a wide range of the needle insertion speed, this paper demonstrates a computational approach that incorporates the surface-based cohesive behavior to simulate a rotating needle cutting soft tissue. The computational model is validated by comparing with a cutting test dataset reported in the literature. The validated model is then used to generate response surfaces of the axial cutting force and torque in a large parameter space of needle rotation and insertion speeds. The results provide guidelines for selecting optimal speed configurations under different design situations.     

Functional roles of the hook in a rotating tethered cell

A bacterial cell tethered through a flagellum on a glass slide rotates its cell body in either counter-clockwise or clockwise at around 10 Hz. To analyze the detailed manner of rotation, we have constructed and expressed yellow fluorescent protein (YFP)-FliN fusion protein in a fliN deletion mutant, resulting in the recovery of motility of the Fla^- mutant cells. The tethered cells that incorporated the fusion protein in the flagellar motor rotate around one of the fluorescent spots. Tracing the center spot of a rotating cell, we have found that the rotating circles of the tethered cells were often distorted, and that the cell has seldom rotated smoothly but gyrated around the center point. The radii of the gyrating circles were 100-200 nm for the wild-type cells, and 50 nm for the cells carrying short hooks, suggesting that the flexibility of the hook is responsible for asymmetrical rotation. These observations indicate that tethered cells almost always interact with the glass surface in one cycle of rotation, where the length and flexibility of the hook have an important role.     

Modulation of the shape and speed of a chemical wave in an unstirred Belousov–Zhabotinsky reaction by a rotating magnet

The objective of this study was to observe whether a rotating magnetic field (RMF) could change the anomalous chemical wave propagation induced by a moderate‐intensity gradient static magnetic field (SMF) in an unstirred Belousov–Zhabotinsky (BZ) reaction. The application of the SMF (maximum magnetic flux density = 0.22 T, maximum magnetic flux density gradient = 25.5 T/m, and peak magnetic force product (flux density × gradient) = 4 T²/m) accelerated the propagation velocity in a two‐dimensional pattern. Characteristic anomalous patterns of the wavefront shape were generated and the patterns were dependent on the SMF distribution. The deformation and increase in the propagation velocity were diminished by the application of an RMF at a rotation rate of 1 rpm for a few minutes. Numerical simulation by means of the time‐averaged value of the magnetic flux density gradient or the MF gradient force over one rotation partially supported the experimental observations. These considerations suggest that RMF exposure modulates the chemical wave propagation and that the degree of modulation could be, at least in part, dependent on the time‐averaged MF distribution over one rotation. Bioelectromagnetics 34:220–230, 2013. © 2012 Wiley Periodicals, Inc.     

Fluctuations in rotation rate of the flagellar motor of Escherichia coli.

The purpose of this work was to study the changes in rotation rate of the bacterial motor and to try to discriminate between various sources of these changes with the aim of understanding the mechanism of force generation better. To this end Escherichia coli cells were tethered and videotaped with brief stroboscopic light flashes. The records were scanned by means of a computerized motion analysis system, yielding cell size, radius of rotation, and accumulated angle of rotation as functions of time for each cell selected. In conformity with previous studies, fluctuations in the rotation rate of the flagellar motor were invariably found. Employing an exclusively counterclockwise rotating mutant ("gutted" RP1091 strain) and using power spectral density, autocorrelation and residual mean square angle analysis, we found that a simple superposition of rotational diffusion on a steady rotary motion is insufficient to describe the observed rotation. We observed two additional rotational components, one fluctuating (0.04-0.6 s) and one oscillating (0.8-7 s). However, the effective rotational diffusion coefficient obtained after taking these two components into account generally exceeded that calculated from external friction by two orders of magnitude. This is consistent with a model incorporating association and dissociation of force-generating units.     

The distribution of fibronectin and laminin in the somitogenesis of Xenopus laevis

Abstract. Two different types of somitogenesis are present in vertebrates. Primarily, somites are formed by segmentation and epithelialization of mesenchyme (rosette formation type). In Xenopus , however, somitogenesis is characterized by a rotation of blocks of mesodermal cells following segmentation. Since this morphogenetic process involves cell movement as well as cell detachment and cell adhesion we analyzed the distribution of fibronectin and laminin in the somitogenesis of Xenopus . For laminin and fibronectin detection we used cross-reacting antibodies. We demonstrated their specific reaction with the Xenopus antigens by Western blots and by immunostainings of different tissues. Tracing both proteins immunohistologically during somitogenesis, our results show that fibronectin appears in the first steps of somitogenesis - during rotation, whereas laminin occurs after somites have already been formed. The different distribution of both proteins during somite formation indicates that fibronectin, but not laminin, is a possible substrate for the rotating cells.     

Design and characterization of a rotating bed system bioreactor for tissue engineering applications

The main challenge in the development of bioreactors for tissue engineering is the delivery of a sufficient nutrient and oxygen supply for cell growth in a 3D environment. Thus, a new rotating bed system bioreactor for tissue engineering applications was developed. The system consists of a culture vessel as well as an integrated rotating bed of special porous ceramic discs and a process control unit connected with the reactor to ensure optimal culturing conditions. The aim of the project was the design and construction of a fully equipped rotating bed reactor, and in particular, the characterization and optimization of the system with regard to technical parameters such as mixing time and pH-control to guarantee optimal conditions for cell growth and differentiation. Furthermore, the applicability of the developed system was demonstrated by cultivation of osteoblast precursor cells. The porous structure of the ceramic discs and the external medium circulation loop provide an optimal environment for tissue generation in long-term cultivations. Mass transfer limitations were minimized by the slow rotation, which also provides the cells with sufficient nutrients and oxygen through alternate contact to air and medium. An osteoblast precursor cell line was successfully cultivated in this bioreactor for 28 days.     

OBSERVATIONS ON METAPHLOEM IN THE VEGETATIVE PARTS OF PALMS

Metaphloem was studied in available vegetative parts of 374 species in 164 genera of palms. Sieve elements usually have compound sieve plates except in the subfamilies Lepidocaryoideae and Nypoideae. Sieve elements in roots usually have oblique to very oblique end walls, whereas in stems and leaves they have transverse to oblique walls. Within a phloem strand the degree of compounding of a sieve plate is directly correlated with element diameter. Plastids are normally present in functioning, enucleate sieve elements. Small quantities of “slime” substances have been detected in young sieve elements in stems and petioles of a few species. Many sieve plates in functioning sieve elements lacked callose in materials quick-killed in liquid nitrogen or chilled acetic-alcohol. Definitive callose is confined to sieve elements just before their obliteration. Sieve tubes in leaf and stem are usually ensheathed by contiguous parenchyma cells while those in root have very few contiguous parenchyma cells. Two types of contiguous parenchyma cells can be distinguished by difference in cytoplasmic density, especially with the electron microscope. Cells with denser cytoplasm are interpreted as companion cells. Lignified contiguous parenchyma cells are occasionally present in metaphloem of petioles. The possible diagnostic and taxonomic features of metaphloem are discussed.     

Thermodynamic battle for photosynthate acquisition between sieve tubes and adjoining parenchyma in transport phloem

In transport phloem, photoassimilates escaping from the sieve tubes are released into the apoplasmic space between sieve element (SE)/companion cell (CC) complexes (SE/CCs) and phloem parenchyma cells (PPCs). For uptake respective retrieval, PPCs and SE/CCs make use of plasma membrane translocators energized by the proton motive force (PMF). Their mutual competitiveness, which essentially determines the amount of photoassimilates translocated through the sieve tubes, therefore depends on the respective PMFs. We measured the components of the PMF, membrane potential and DeltapH, of SE/CCs and PPCs in transport phloem. Membrane potentials of SE/CCs and PPCs in tissue slices as well as in intact plants fell into two categories. In the first group including apoplasmically phloem-loading species (e.g. Vicia, Solanum), the membrane potentials of the SEs are more negative than those of the PPCs. In the second group including symplasmically phloem-loading species (e.g. Cucurbita, Ocimum), membrane potentials of SEs are equal to or slightly more positive than those of PPCs. Pure sieve tube sap collected from cut aphid stylets was measured with H(+)-selective microelectrodes. Under our experimental conditions, pH of the sieve tube saps was around 7.5, which is comparable to the pH of cytoplasmic compartments in parenchymatous cells. In conclusion, only the membrane potential appears to be relevant for the PMF-determined competition between SE/CCs and PPCs. The findings may imply that the axial sinks along the pathway withdraw more photoassimilates from the sieve tubes in symplasmically loading species than in apoplasmically loading species.     

Real time computer tracking of free-swimming and tethered rotating cells

A computerized image processing system has been developed that tracks individual free-swimming cells and rotating bacterial cell bodies tethered by their flagella in real time. Free-swimming bacteria of Rhodobacter sphaeroides, Rhodospirullum rubrum, and Salmonella typhimurium have been tracked swimming at speeds from 0 to over 120 microns s-1. A high level of discrimination is exerted against noncellular objects, allowing analysis of stopped as well as moving cells. This enabled detection of both speed and qualitative change in the swimming patterns of R. sphaeroides WS8 upon tactic stimulation. Comparison with darkfield microscopy indicated that the two techniques were in substantial agreement. The unidirectional rotation of cells of R. sphaeroides WS8 could be detected when the cells were either parallel to the microscope slide or end on. Frequencies of rotation of up to 10 Hz were monitored before image blurring became a problem. True rods would be easier to analyze at higher speeds of rotation. Although developed for photosynthetic bacteria, a wide range of bacteria, eucaryotic organisms, and subcellular organelles could be tracked with this system. Minor modifications to the software allow customization to different types of motility analysis.     

Symmetrically dividing cell specific division axes alteration observed in proteasome depleted C. elegans embryo

A fertilised Caenorhabditis elegans embryo shows an invariable pattern of cell division and forms a multicellular body where each cell locates to a defined position. Mitotic spindle orientation is determined by several preceding events including the migration of duplicated centrosomes on a nucleus and the rotation of nuclear-centrosome complex. Cell polarity is the dominant force driving nuclear-centrosome rotation and setting the mitotic spindle axis in parallel with the polarity axis during asymmetric cell division. It is reasonable that there is no nuclear-centrosome rotation in symmetrically dividing blastomeres, but the mechanism(s) which suppress rotation in these cells have been proposed because the rotations occur in some polarity defect embryos. Here we show the nuclear-centrosome rotation can be induced by depletion of RPN-2, a regulatory subunit of the proteasome. In these embryos, cell polarity is established normally and both asymmetrically and symmetrically dividing cells are generated through asymmetric cell divisions. The nuclear-centrosome rotations occurred normally in the asymmetrically dividing cell lineage, but also induced in symmetrically dividing daughter cells. Interestingly, we identified RPN-2 as a binding protein of PKC-3, one of critical elements for establishing cell polarity during early asymmetric cell divisions. In addition to asymmetrically dividing cells, PKC-3 is also expressed in symmetrically dividing cells and a role to suppress nuclear-centrosome rotation has been anticipated. Our data suggest that the expression of RPN-2 is involved in the mechanism to suppress nuclear-centrosome rotation in symmetrically dividing cells and it may work in cooperation with PKC-3.     

Generalization of Dexterous Manipulation Is Sensitive to the Frame of Reference in Which It Is Learned

Studies have shown that internal representations of manipulations of objects with asymmetric mass distributions that are generated within a specific orientation are not generalizable to novel orientations, i.e., subjects fail to prevent object roll on their first grasp-lift attempt of the object following 180° object rotation. This suggests that representations of these manipulations are specific to the reference frame in which they are formed. However, it is unknown whether that reference frame is specific to the hand, the body, or both, because rotating the object 180° modifies the relation between object and body as well as object and hand. An alternative, untested explanation for the above failure to generalize learned manipulations is that any rotation will disrupt grasp performance, regardless if the reference frame in which the manipulation was learned is maintained or modified. We examined the effect of rotations that (1) maintain and (2) modify relations between object and body, and object and hand, on the generalizability of learned two-digit manipulation of an object with an asymmetric mass distribution. Following rotations that maintained the relation between object and body and object and hand (e.g., rotating the object and subject 180°), subjects continued to use appropriate digit placement and load force distributions, thus generating sufficient compensatory moments to minimize object roll. In contrast, following rotations that modified the relation between (1) object and hand (e.g. rotating the hand around to the opposite object side), (2) object and body (e.g. rotating subject and hand 180°), or (3) both (e.g. rotating the subject 180°), subjects used the same, yet inappropriate digit placement and load force distribution, as those used prior to the rotation. Consequently, the compensatory moments were insufficient to prevent large object rolls. These findings suggest that representations of learned manipulation of objects with asymmetric mass distributions are specific to the body- and hand-reference frames in which they were learned.     

Influence of environmental factors on shot put and hammer throw range

On the rotating Earth, in addition to the Newtonian gravitational force, two additional relevant inertial forces are induced, the centrifugal and Coriolis forces. Using computer modelling for typical release heights and optimal release angles, we compare the influence of Earth rotation on the range of the male hammer throw and shot put with that of air resistance, wind, air pressure and temperature, altitude and ground obliquity. Practical correction maps are presented, by which the ranges achieved at different latitudes and/or with different release directions can be corrected by a term involving the effect of Earth rotation. Our main conclusion and suggestion is that the normal variations of certain environmental factors can be substantially larger than the smallest increases in the world records as acknowledged by the International Amateur Athletic Federation and, therefore, perhaps these should be accounted for in a normalization and adjustment of the world records to some reference conditions. Although this suggestion has certainly been made before, the comprehensiveness of our study makes it even more compelling. Our numerical calculations contribute to the comprehensive understanding and tabulation of these effects, which is largely lacking today.     

Vascular Anatomy of Angiospermous Leaves,with Special Consideration of the Maize Leaf

In this brief review an attempt has been made to discuss some of the important features of the vascular anatomy of angiospermous leaves, especially those related to assimilate transport. Accordingly, emphasis has been placed on the small or minor veins, which are closely related spatially to the mesophyll, and which play a major role in the uptake and subsequent transport of photosynthates from the leaf. The small veins are enclosed by bundle sheaths that intervene between the mesophyll and vascular tissues and greatly increase the area for contact with mesophyll cells. In the minor veins of dicotyledonous leaves, parenchymatic cells having organelle-rich protoplasts and numerous cytoplasmic connections with sieve elements dominate quantitatively. It is these so-called intermediary cells that apparently are directly involved with the loading of assimilates into the sieve elements. In the maize leaf the small and intermediate bundles have two types of sieve tubes, relatively thin-walled ones that have numerous cytoplasmic connections with companion cells, and thick-walled ones that lack companion cells but have numerous connections with vascular parenchyma cells. The companion cell-sieve tube complexes are virtually isolated symplastically from other cells of the vascular bundle and from the bundle sheath. Thick-walled sieve tubes similar to those in the maize leaf have been recorded in the leaves of other grasses.     

On torque and tumbling in swimming Escherichia coli

Bacteria swim by rotating long thin helical filaments, each driven at its base by a reversible rotary motor. When the motors of peritrichous cells turn counterclockwise (CCW), their filaments form bundles that drive the cells forward. We imaged fluorescently labeled cells of Escherichia coli with a high-speed charge-coupled-device camera (500 frames/s) and measured swimming speeds, rotation rates of cell bodies, and rotation rates of flagellar bundles. Using cells stuck to glass, we studied individual filaments, stopping their rotation by exposing the cells to high-intensity light. From these measurements we calculated approximate values for bundle torque and thrust and body torque and drag, and we estimated the filament stiffness. For both immobilized and swimming cells, the motor torque, as estimated using resistive force theory, was significantly lower than the motor torque reported previously. Also, a bundle of several flagella produced little more torque than a single flagellum produced. Motors driving individual filaments frequently changed directions of rotation. Usually, but not always, this led to a change in the handedness of the filament, which went through a sequence of polymorphic transformations, from normal to semicoiled to curly 1 and then, when the motor again spun CCW, back to normal. Motor reversals were necessary, although not always sufficient, to cause changes in filament chirality. Polymorphic transformations among helices having the same handedness occurred without changes in the sign of the applied torque.     

The Flat-Ribbon Configuration of the Periplasmic Flagella of Borrelia burgdorferi and Its Relationship to Motility and Morphology

Electron cryotomography was used to analyze the structure of the Lyme disease spirochete, Borrelia burgdorferi. This methodology offers a new means for studying the native architecture of bacteria by eliminating the chemical fixing, dehydration, and staining steps of conventional electron microscopy. Using electron cryotomography, we noted that membrane blebs formed at the ends of the cells. These blebs may be precursors to vesicles that are released from cells grown in vivo and in vitro. We found that the periplasmic space of B. burgdorferi was quite narrow (16.0 nm) compared to those of Escherichia coli and Pseudomonas aeruginosa. However, in the vicinity of the periplasmic flagella, this space was considerably wider (42.3 nm). In contrast to previous results, the periplasmic flagella did not form a bundle but rather formed a tight-fitting ribbon that wraps around the protoplasmic cell cylinder in a right-handed sense. We show how the ribbon configuration of the assembled periplasmic flagella is more advantageous than a bundle for both swimming and forming the flat-wave morphology. Previous results indicate that B. burgdorferi motility is dependent on the rotation of the periplasmic flagella in generating backward-moving waves along the length of the cell. This swimming requires that the rotation of the flagella exerts force on the cell cylinder. Accordingly, a ribbon is more beneficial than a bundle, as this configuration allows each periplasmic flagellum to have direct contact with the cell cylinder in order to exert that force, and it minimizes interference between the rotating filaments.