Rapid backward movement of anaphase chromosome whose kinetochore fibers were cut by ultraviolet microbeam irradiation

Summary— kinetochore spindle fibers in meiosis I and II grasshopper spermatocytes were cut with a heterochromatic ultraviolet (UV) microbeam converging on the specimen to form a slit-shaped microspot 1.5 × 8 μm or 3 × 8 μm. A total exposure of 3 × 10^?8 joules per μm² was administered within 0.8–2.4 s, which was sufficient for severing. The cells were observed with a high extinction polarizing microscope or phase contrast optics and a record made by time-lapse video microscopy, continuously before, during and after the irradiation. When kinetochore fibers were irradiated i anaphase with UV, an area of reduced birefringence (ARB) was produced at the exposed site. The newly created + ends of the microtubules rapidly disassembled poleward, at a constant speed of 17 μm/min. The — ends at the edge of ARB also depolymerized at a slower rate. When a kinetochore fiber was cut with UV in early anaphase at which time its associated chromosome had not disjoined from the partner chromosome, the chromosome of the irradiated kinetochore fiber moved rapidly back to its partner. The speed during this movement was faster than the normal poleward chromosome movement in anaphase by an order to magnitude or more. When a kinetochore and its associated kinetochore fiber were included in the irradiation are, the effects were more pronounced than the effects of irradiation on a kinetochore fiber alone; the direction of the line connecting the irradiated half-bivalent with the partner half-bivalent deviated so much from the longitudinal axis of the original spindle with time that the division assumed a tripolar figure.     

Characterization of the mitotic traction system,and evidence that birefringent spindle fibers neither produce nor transmit force for chromosome movement

Living crane fly spermatocytes were irradiated in various areas, and changes in chromosome movement and changes in spindle fiber birefringence were measured.The traction system was localized in the chromosomal spindle fibers; an undamaged traction fiber extending at least 1/2 the fiber length (from the chromosome) is necessary for normal movement. The results suggest, however, that the birefringent fiber is separate from the traction fiber, and therefore that the chromosomal spindle fiber is composed of at least 2 components. Otherwise, the following results characterize the traction fiber: birefringence is not necessary for movement, birefringence and movement are affected independently, the birefringent fiber moves poleward when the associated chromosome does not move, and the birefringent fiber moves poleward at a rate not related to that of the associated chromosome. These and other results are more easily explained under the assumptions: (1) during anaphase, the birefringent fiber is independent of the traction fiber, and (2) prior to anaphase, the birefringent fiber is not independent of the traction fiber.The traction system was further characterized as follows: the anaphase movements of sister dyads are interdependent; in a cell, different sister dyad pairs are independent during anaphase but are not independent prior to anaphase; the initial separation of dyads is autonomous; the spindle organization changes markedly between metaphase and anaphase; and, something in the interzonal region is necessary for the subsequent division.It was suggested that the interdependent movement of sister dyads is mediated via functioning kinetochores. It was further suggested that this interdependence is mediated via kinetochore-interzonal region interactions, and that the interzonal region is involved with regulating the amount of force on the chromosome.Portions of this paper were presented to Dartmouth College in partial fullfilment of the requirements for the degree of Doctor of Philosophy.     

Structure of kinetochore fibres in crane-fly spermatocytes after irradiation with an ultraviolet microbeam: neither microtubules nor actin filaments remain in the irradiated region

We studied chromosome movement after kinetochore microtubules were severed. Severing a kinetochore fibre in living crane-fly spermatocytes with an ultraviolet microbeam creates a kinetochore stub, a birefringent remnant of the spindle fibre connected to the kinetochore and extending only to the edge of the irradiated region. After the irradiation, anaphase chromosomes either move poleward led by their stubs or temporarily stop moving. We examined actin and/or microtubules in irradiated cells by means of confocal fluorescence microscopy or serial-section reconstructions from electron microscopy. For each cell thus examined, chromosome movement had been recorded continuously until the moment of fixation. Kinetochore microtubules were completely severed by the ultraviolet microbeam in cells in which chromosomes continued to move poleward after the irradiation: none were seen in the irradiated regions. Similarly, actin filaments normally present in kinetochore fibres were severed by the ultraviolet microbeam irradiations: the irradiated regions contained no actin filaments and only local spots of non-filamentous actin. There was no difference in irradiated regions when the associated chromosomes continued to move versus when they stopped moving. Thus, one cannot explain motion with severed kinetochore microtubules in terms of either microtubules or actin-filaments bridging the irradiated region. The data seem to negate current models for anaphase chromosome movement and support a model in which poleward chromosome movement results from forces generated within the spindle matrix that propel kinetochore fibres or kinetochore stubs poleward.     

Micromanipulation studies of chromosome movement. II. Birefringent chromosomal fibers and the mechanical attachment of chromosomes to the spindle

The degree of mechanical coupling of chromosomes to the spindles of Nephrotoma and Trimeratropis primary spermatocytes varies with the stage of meiosis and the birefringent retardation of the chromosomal fibers. In early prometaphase, before birefringent chromosomal fibers have formed, a bivalent can be displaced toward a spindle pole by a single, continuous pull with a microneedle. Resistance to poleward displacement increases with increased development of the chromosomal fibers, reaching a maximum at metaphase. At this stage kinetochores cannot be displaced greater than 1 micrometer toward either spindle pole, even by a force which is sufficient to displace the entire spindle within the cell. The abolition of birefringence with either colcemid or vinblastine results in the loss of chromosome-spindle attachment. In the absence of birefringent fibers a chromosome can be displaced anywhere within the cell. The photochemical inactivation of colcemid by irradiation with 366-nm light results in the reformation of birefringent chromosomal fibers and the concomitant re-establishment of chromosome attachment to the spindle. These results support the hypothesis that the birefringent chromosomal fibers anchor the chromosomes to the spindle and transmit the force for anaphase chromosome movement.     

Mitosis in Tilia americana endosperm

The endosperm cells of the American basswood Tilia americana are favorable experimental material for investigating the birefringence of living plant spindles and anaphase movement of chromosomes. The behavior of the chromosomes in anaphase and the formation of the phragmoplast are unique. The numerous (3 n equals 123), small chromosomes move in precise, parallel rows until midanaphase when they bow away from the poles. Such a pattern of anaphase chromosome distribution has been described once before, but was ascribed to fusion of the chromosomes. The bowing of chromosome rows in Tilia is explainable quantitatively by the constant poleward velocity of the chromosomes during anaphase. Peripheral chromosomes are moving both relative to the spindle axis and laterally closer to the axis, whereas chromosomes lying on the spindle axis possess no lateral component in their motion, and thus at uniform velocity progress more rapidly than peripheral chromosomes relative to the spindle axis. The chromosomes are moved poleward initially by pole-to-pole elongation of the spindle, then moved farther apart by shortening of the kinetochore fibers. In contrast to other plant cells where the phragmoplast forms in telophase, the phragmoplast in Tilia endosperm is formed before midanaphase and the cell during midanaphase, while the chromosomes are still in poleward transit.     

The motor for poleward chromosome movement in anaphase is in or near the kinetochore

I have tested two contending views of chromosome-to-pole movement in anaphase. Chromosomes might be pulled poleward by a traction fiber consisting of the kinetochore microtubules and associated motors, or they might propel themselves by a motor in the kinetochore. I cut through the spindle of demembranated grasshopper spermatocytes between the chromosomes and one pole and swept the polar region away, removing a portion of the would-be traction fiber. Chromosome movement continued, and in the best examples, chromosomes moved to within 1 micron of the cut edge. There is nothing beyond the edge to support movement, and a push from the rear is unlikely because cuts in the interzone behind the separating chromosomes did not stop movement. Therefore, I conclude that the motor must be in the kinetochore or within 1 micron of it. Less conclusive evidence points to the kinetochore itself as the motor. The alternative is an external motor pulling on the kinetochore microtubules or directly on the kinetochore. A pulling motor would move kinetochore microtubules along with the chromosome, so that in a cut half-spindle, the microtubules should protrude from the cut edge as chromosomes move toward it. No protrusion was seen; however, the possibility that microtubules depolymerize as they are extruded, though unlikely, is not ruled out. What is certain is that the motor for poleward chromosome movement in anaphase must be in the kinetochore or very close to it.     

UV microbeam irradiations of the mitotic spindle. II. Spindle fiber dynamics and force production

Metaphase and anaphase spindles in cultured newt and PtK1 cells were irradiated with a UV microbeam (285 nM), creating areas of reduced birefringence (ARBs) in 3 s that selectively either severed a few fibers or cut across the half spindle. In either case, the birefringence at the polewards edge of the ARB rapidly faded polewards, while it remained fairly constant at the other, kinetochore edge. Shorter astral fibers, however, remained present in the enlarged ARB; presumably these had not been cut by the irradiation. After this enlargement of the ARB, metaphase spindles recovered rapidly as the detached pole moved back towards the chromosomes, reestablishing spindle fibers as the ARB closed; this happened when the ARB cut a few fibers or across the entire half spindle. We never detected elongation of the cut kinetochore fibers. Rather, astral fibers growing from the pole appeared to bridge and then close the ARB, just before the movement of the pole toward the chromosomes. When a second irradiation was directed into the closing ARB, the polewards movement again stopped before it restarted. In all metaphase cells, once the pole had reestablished connection with the chromosomes, the unirradiated half spindle then also shortened to create a smaller symmetrical spindle capable of normal anaphase later. Anaphase cells did not recover this way; the severed pole remained detached but the chromosomes continued a modified form of movement, clumping into a telophase-like group. The results are discussed in terms of controls operating on spindle microtubule stability and mechanisms of mitotic force generation.     

Temperature dependence of anaphase chromosome velocity and microtubule depolymerization

The time course of chromosome movement and decay of half-spindle birefringence retardation in anaphase have been precisely determined in the endosperm cell of a plant Tilia americana and in the egg of an animal Asterias forbesi. For each species, the anaphase retardation decay rate constant and chromosome velocity are similar exponential functions of temperature. Over the temperature range at which these cells can complete anaphase, chromosome velocity and retardation rate constant yield a positive linear relationship when plotted against each other. At the higher temperatures where the chromosomes move faster, the spindle retardation decays faster, even though the absolute spindle retardation is greater. Chromosome velocity thus parallels the anaphase spindle retardation decay rate, or rate of spindle microtubule depolymerization, rather than absolute spindle retardation, or the amount of microtubules in the spindle. These observations suggest that a common mechanism exists for mitosis in plant and animal cells. The rate of anaphase chromosome movement is associated with an apparent first-order process of spindle fiber disassembly. This process irreversibly prevents spindle fiber subunits from participating in the polymerization equilibrium and removes microtubular subunits from chromosomal spindle fibers.     

Morphological studies on the structure of univalent sex chromosomes during anaphase movement in spermatocytes of the crane fly Pales ferruginea

The ultrastructure of moving amphitelic sex chromosomes during anaphase of the first meiotic division of spermatocytes was studied by means of serial sections. The chromosomes have radial lamellae-like projections at their surface running in the direction of the spindle axis. Parallel spindle microtubules lie between these lamellae. The kinetochoral region pointing to the interzone (K_IZ) is stretched, while the kinetochore pointing polewards (K_p) is flat. It is suggested that the importance of the poleward kinetochore as an application site for pulling forces during anaphase movement is possibly reduced in favour of the lamellaemicrotubule association at the periphery of the chromosome. Distal parts of kinetochoral tubules of K_IZ may be associated with the lamellae of the partner sex chromosome. This arrangement may have some additional importance for the synchronization of sex chromosome migration in anaphase.     

Direct visualization of microtubule flux during metaphase and anaphase in crane-fly spermatocytes

Microtubule flux in spindles of insect spermatocytes, long-used models for studies on chromosome behavior during meiosis, was revealed after iontophoretic microinjection of rhodamine-conjugated (rh)-tubulin and fluorescent speckle microscopy. In time-lapse movies of crane-fly spermtocytes, fluorescent speckles generated when rh-tubulin incorporated at microtubule plus ends moved poleward through each half-spindle and then were lost from microtubule minus ends at the spindle poles. The average poleward velocity of approximately 0.7 microm/min for speckles within kinetochore microtubules at metaphase increased during anaphase to approximately 0.9 microm/min. Segregating half-bivalents had an average poleward velocity of approximately 0.5 microm/min, about half that of speckles within shortening kinetochore fibers. When injected during anaphase, rhtubulin was incorporated at kinetochores, and kinetochore fiber fluorescence spread poleward as anaphase progressed. The results show that tubulin subunits are added to the plus end of kinetochore microtubules and are removed from their minus ends at the poles, all while attached chromosomes move poleward during anaphase A. The results cannot be explained by a Pac-man model, in which 1) kinetochore-based, minus end-directed motors generate poleward forces for anaphase A and 2) kinetochore microtubules shorten at their plus ends. Rather, in these cells, kinetochore fiber shortening during anaphase A occurs exclusively at the minus ends of kinetochore microtubules.     

Mitosis in Barbulanympha. II. Dynamics of a two-stage anaphase, nuclear morphogenesis, and cytokinesis

Anaphase in Barbulanympha proceeds in two discrete steps. In anaphase- A, chromosomal spindle fibers shorten and chromosomes move to the stationary centrosomes. In anaphase-B, the central spindle elongates and ("telophasic") bouquets of chromosomes, with kinetochores still connected by the shortened chromosomal fibers to the centrosomes, are moved far apart. The length, width, and birefringence of the central spindle remain unchanged throughout anaphase-A. In anaphase-B, the central spindle elongates up to fivefold. During elongation, the peripheral fibers of the central spindle splay, first anteriorly and then laterally. The remaining central spindle progressively becomes thinner and the retardation decreases; however, the coefficient of birefringence stays approximately constant. The nuclear envelope persists throughout mitosis in Barbulanympha and the nucleus undergoes an intricate morphological change. In prophase, the nucleus engulfs the spindle; in early anaphase-A, the nuclear envelope forms a seam anterior to the spindle, the nucleus thus transforms into a complete sleeve surrounding the central spindle. In late anaphase-A, the middle of the seam opens up in a cleft as the lips part; in anaphase-B, the cleft expands posteriorly, progressively exposing the central spindle. Finally, the cleft partitions the nucleus into two. The nuclear envelope shows an apparent elasticity and two-dimensional fluidity. Localized, transient deformations of the nuclear envelope indicate poleward and counter-poleward forces acting on the kinetochores embedded in the envelope. These forces appear responsible for nuclear morphogenesis as well as anaphase chromosome movement. At the end of anaphase-B, the two rostrate Barbulanympha may swim apart of be poked apart into two daughter cells by another organism cohabiting the host's hindgut.     

Polar ejection forces are operative in crane-fly spermatocytes, but their action is limited to the spindle periphery.

Laser microsurgery was employed to reveal kinetochore-independent forces acting on chromosome arms in crane-fly spermatocytes. When a portion of an arm situated along the interpolar axis between the equator and a pole was cut off, the resultant acentric fragment was transported poleward and outward into the peripheral domain of the spindle. If the fragment was generated well in advance of the onset of anaphase, then at the spindle periphery, it changed direction and moved away from the pole and back toward the equator. That domain-specific movement-poleward in the central spindle and away from the pole at the spindle periphery-not only provides the first evidence for polar ejection forces acting on acentric fragments in a meiotic system, but it is the first example of kinetochore-independent forces in both directions at the same stage of division. Sniglets generated by laser pulses directed at specific sites in the spindle revealed that the mechanism underlying ejection forces was specific to chromosomes. At anaphase onset, polar ejection forces ceased, and pole-directed forces took over. At that time, chromosome fragments that had been ejected to the equator moved poleward again, providing clear evidence for kinetochore-independent forces on chromosome arms during anaphase.     

Rhodamine-phalloidin and anti-tubulin antibody staining of spindle fibres that were irradiated with an ultraviolet microbeam

Summary We irradiated chromosomal spindle fibres in crane-fly spermatocytes with an ultraviolet microbeam of 270 nm wavelength light with total energies near those that cause actin filaments in myofibrils to depolymerize; after irradiation we stained the cells with rhodamine-labelled phalloidin and with anti-tubulin antibodies. In some cells, the irradiation reduced both phalloidin and tubulin staining of the chromosomal spindle fibres; in other cells, the irradiations reduced phalloidin staining but not tubulin staining; in yet other cells, the irradiations reduced tubulin staining but not phalloidin staining. In all irradiated cells in which phalloidin staining was reduced in the irradiated areas phalloidin staining also was reduced poleward from the irradiated areas. These results show that phalloidin staining of chromosomal spindle fibres is not dependent on the presence of kinetochore microtubules, and, therefore, that actin filaments are present in the spindle fibres in vivo. We suggest that actin filaments present in spindle fibres in vivo may be involved in causing chromosome movements during anaphase.     

The reduction of chromosome number in meiosis is determined by properties built into the chromosomes

In meiosis I, two chromatids move to each spindle pole. Then, in meiosis II, the two are distributed, one to each future gamete. This requires that meiosis I chromosomes attach to the spindle differently than meiosis II chromosomes and that they regulate chromosome cohesion differently. We investigated whether the information that dictates the division type of the chromosome comes from the whole cell, the spindle, or the chromosome itself. Also, we determined when chromosomes can switch from meiosis I behavior to meiosis II behavior. We used a micromanipulation needle to fuse grasshopper spermatocytes in meiosis I to spermatocytes in meiosis II, and to move chromosomes from one spindle to the other. Chromosomes placed on spindles of a different meiotic division always behaved as they would have on their native spindle; e.g., a meiosis I chromosome attached to a meiosis II spindle in its normal fashion and sister chromatids moved together to the same spindle pole. We also showed that meiosis I chromosomes become competent meiosis II chromosomes in anaphase of meiosis I, but not before. The patterns for attachment to the spindle and regulation of cohesion are built into the chromosome itself. These results suggest that regulation of chromosome cohesion may be linked to differences in the arrangement of kinetochores in the two meiotic divisions.     

UV-microbeam irradiations of the mitotic spindle: spindle forces and structural analysis of lesions

Mitotic PtK1 spindles were UV irradiated (285 nm) during metaphase and anaphase between the chromosomes and the pole. The irradiation, a rectangle measuring 1.4 x 5 microns parallel to the metaphase plate, severed between 90 and 100% of spindle microtubules (MTs) in the irradiated region. Changes in organization of MTs in the irradiated region were analyzed by EM serial section analysis coupled with 3-D computer reconstruction. Metaphase cells irradiated 2 to 4 microns below the spindle pole (imaged by polarization optics) lost birefringence in the irradiated region. Peripheral spindle fibers, previously curved to focus on the pole, immediately splayed outwards when severed. We demonstrate via serial section analysis that following irradiation the lesion was devoid of MTs. Within 30 s to 1 min, recovery in live cells commenced as the severed spindle pole moved toward the metaphase plate closing the lesion. This movement was concomitant with the recovery of spindle birefringence and some of the severed fibers becoming refocused at the pole. Ultrastructurally we confirmed that this movement coincided with bridging of the lesion by MTs presumably growing from the pole. The non-irradiated half spindle also lost some birefringence and shortened until it resembled the recovered half spindle. Anaphase cells similarly irradiated did not show recovery of birefringence, and the pole remained disconnected from the remaining mitotic apparatus. Reconstructions of spindle structure confirmed that there were no MTs in the lesion which bridged the severed spindle pole with the remaining mitotic apparatus. These results suggest the existence of chromosome-to-pole spindle forces are dependent upon the existence of a MT continuum, and to a lesser extent to the loss of MT initiation capacity of the centrosome at the metaphase/anaphase transition.     

Functional implications of cold-stable microtubules in kinetochore fibers of insect spermatocytes during anaphase

In normal anaphase of crane fly spermatocytes, the autosomes traverse most of the distance to the poles at a constant, temperature-dependent velocity. Concurrently, the birefringent kinetochore fibers shorten while retaining a constant birefringent retardation (BR) and width over most of the fiber length as the autosomes approach the centrosome region. To test the dynamic equilibrium model of chromosome poleward movement, we abruptly cooled or heated primary spermatocytes of the crane fly Nephrotoma ferruginea (and the grasshopper Trimerotropis maritima) during early anaphase. According to this model, abrupt cooling should induce transient depolymerization of the kinetochore fiber microtubules, thus producing a transient acceleration in the poleward movement of the autosomal chromosomes, provided the poles remain separated. Abrupt changes in temperature from 22 degrees C to as low as 4 degrees C or as high as 31 degrees C in fact produced immediate changes in chromosome velocity to new constant velocities. No transient changes in velocity were observed. At 4 degrees C (10 degrees C for grasshopper cells), chromosome movement ceased. Although no nonkinetochore fiber BR remained at these low temperatures, kinetochore fiber BR had changed very little. The cold stability of the kinetochore fiber microtubules, the constant velocity character of chromosome movement, and the observed Arrhenius relationship between temperature and chromosome velocity indicate that a rate-limiting catalyzed process is involved in the normal anaphase depolymerization of the spindle fiber microtubules. On the basis of our birefringence observations, the kinetochore fiber microtubules appear to exist in a steady-state balance between comparatively irreversible, and probably different, physiological pathways of polymerization and depolymerization.     

Poleward microtubule flux is a major component of spindle dynamics and anaphase a in mitotic Drosophila embryos

During cell division, eukaryotic cells assemble dynamic microtubule-based spindles to segregate replicated chromosomes. Rapid spindle microtubule turnover, likely derived from dynamic instability, has been documented in yeasts, plants and vertebrates. Less studied is concerted spindle microtubule poleward translocation (flux) coupled to depolymerization at spindle poles. Microtubule flux has been observed only in vertebrates, although there is indirect evidence for it in insect spermatocytes and higher plants. Here we use fluorescent speckle microscopy (FSM) to demonstrate that mitotic spindles of syncytial Drosophila embryos exhibit poleward microtubule flux, indicating that flux is a widely conserved property of spindles. By simultaneously imaging chromosomes (or kinetochores) and flux, we provide evidence that flux is the dominant mechanism driving chromosome-to-pole movement (anaphase A) in these spindles. At 18 degrees C and 24 degrees C, separated sister chromatids moved poleward at average rates (3.6 and 6.6 microm/min, respectively) slightly greater than the mean rates of poleward flux (3.2 and 5.2 microm/min, respectively). However, at 24 degrees C the rate of kinetochore-to-pole movement varied from slower than to twice the mean rate of flux, suggesting that although flux is the dominant mechanism, kinetochore-associated microtubule depolymerization contributes to anaphase A.     

Chromosome micromanipulation

Two types of unusual motion within the spindle have heen studied in a grasshopper (Melanoplus differentialis) spermatocyte. The first is the motion of granules placed by micromanipulation within the normally granule-free spindle. The most specific motions are poleward, approximate the speed of the chromosomes in anaphase, and occur in the area between the kinetochores and the nearer pole during both metaphase and anaphase. Exactly the same transport properties were earlier observed by Bajer inHaemanthus endosperm spindles. The absence of significant motion in the interzone between the separating chromosomes at anaphase has been unequivocally demonstrated inMelanoplus spermatocytes. Thus very specific motion of non-kinetochoric materials is probably a general spindle capability which would much restrict admissible models of mitotic force production,if the same forces move both granules and chromosomes. The second unusual motion is seen following chromosome detachment from the spindle by micromanipulation during anaphase. These tend to move toNearer pole rather than to the pole the chromosome's kinetochoresFace. The latter preference was earlier demonstrated after detachment during prometaphase or metaphase and has been confirmed without exception in the present studies. The apparent preference for motion to the nearer pole in anaphase provides the first evidence for poleward forces within each half-spindle which cannot be entirely specified by the chromosomal spindle fibers. Almost certainly these would be the usual forces responsible for chromosome motion since they act specifically at the kinetochores of detached chromosomes. This evidence requires interpretation, however because additional factors influence chromosome motion following detachment at anaphase. On thesimplest interpretation, certain current models of mitosis clearly are not satisfactory and others are favored.     

Ultraviolet microbeam irradiations of spindle fibres in crane-fly spermatocytes and newt epithelial cells: Resolution of previously conflicting observations

Summary In order to resolve apparent differences in reported experiments, we directly compared the effects of ultraviolet (UV) microbeam irradiations on the behaviour of spindle fibres in newt epithelial cells and crane-fly spermatocytes, using the same apparatus for both cell types. This work represents the first time that irradiated crane-fly spermatocytes have been followed using a high-NA objective and video-enhancement of images. In both cell types, irradiation of a kinetochore fibre in metaphase produced an area of reduced birefringence (ARB), known to be devoid of spindle microtubules (MTs). Subsequently the kinetochore-ward edge of the ARB moved poleward with average velocities of 0.5 m/min (n=20) in spermatocytes and 1.1 m/min (n=6) in epithelial cells. The poleward edge of the ARB rapidly disappeared when viewed using a ×100, high-NA objective but generally remained visible when viewed with a ×32, low-NA objective; this difference suggests that MTs poleward from the ARB disperse vertically out of the narrow depth of field of the ×100 objective but that many remain encompassed by that of the ×32 objective. The primary difference in response between the two cell types was in the behaviour of the spindle poles after an ARB formed. In spermatocytes the spindle maintained its original length whereas in epithelial cells the pole on the irradiated side very soon moved towards the chromosomes, after which the other pole did the same and a much shortened functional metaphase spindle was formed.     

Microtubule Flux Mediates Poleward Motion of Acentric Chromosome Fragments during Meiosis in Insect Spermatocytes

We applied a combination of laser microsurgery and quantitative polarization microscopy to study kinetochore-independent forces that act on chromosome arms during meiosis in crane fly spermatocytes. When chromosome arms located within one of the half-spindles during prometa- or metaphase were cut with the laser, the acentric fragments (lacking kinetochores) that were generated moved poleward with velocities similar to those of anaphase chromosomes (approximately 0.5 microm/min). To determine the mechanism underlying this poleward motion of detached arms, we treated spermatocytes with the microtubule-stabilizing drug taxol. Spindles in taxol-treated cells were noticeably short, yet with polarized light, the distribution and densities of microtubules in domains where fragment movement occurred were not different from those in control cells. When acentric fragments were generated in taxol-treated spermatocytes, 22 of 24 fragments failed to exhibit poleward motion, and the two that did move had velocities attenuated by 80% (to approximately 0.1 microm/min). In these cells, taxol did not inhibit the disjunction of chromosomes nor prevent their poleward segregation during anaphase, but the velocity of anaphase was also decreased 80% (approximately 0.1 microm/min) relative to untreated controls. Together, these data reveal that microtubule flux exerts pole-directed forces on chromosome arms during meiosis in crane fly spermatocytes and strongly suggest that the mechanism underlying microtubule flux also is used in the anaphase motion of kinetochores in these cells.