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An actomyosin ring is a contractile assembly containing actin filaments and myosin II. In typical animal cytokinesis, it forms in the cell cortex beneath the cell membrane. Its contraction draws the boundary inward to produce a cleavage furrow; an inward groove is not yet complete separation of the daughters.^[ref]

Myosin II participates in the actomyosin ring of typical animal cytokinesis.^[ref]

Myosins convert a nucleotide-driven actin-binding cycle into movement, force or anchoring. Their different cellular roles arise from variations in motor kinetics, directionality, lever-arm geometry, oligomerization and cargo binding. A class name alone does not specify a universal stepping speed or duty ratio.

A myosin usually contains an actin-binding motor domain with an ATPase active site, a neck associated with light chains, and a tail involved in cargo association or assembly. The myosin lever arm amplifies small motor-domain rearrangements. The tail can connect the motor to a membrane, receptor, organelle or another myosin molecule. Some isoforms are autoinhibited until cargo binding, calcium-dependent regulation or phosphorylation favours an active conformation.

The mechanochemical cycle can be organized around actin affinity. In a strongly bound nucleotide-free state, ATP binding weakens actin attachment and promotes detachment. ATP hydrolysis prepares a detached or weakly bound ADP–phosphate state. Subsequent actin interaction and transitions around phosphate release stabilize strong binding and generate the myosin power stroke. ADP release and the next ATP-binding event complete the cycle. The exact ordering and rates of structural transitions and phosphate release depend on isoform and load; the cycle should not be reduced to a claim that ATP cleavage itself is the instantaneous mechanical stroke.

Directionality depends on motor geometry and the polarity of actin. Most characterized myosins move toward the barbed end, but Myosin VI moves toward the pointed end. Motor assays established this reversed direction directly, showing that “myosin” does not imply a single transport direction.^[ref] In a cortex with complex actin architecture, filament orientation must therefore be known before predicting net cargo movement.

The myosin duty ratio is the fraction of a cycle spent strongly bound. A single low-duty motor repeatedly loses its track, whereas an assembly of many such motors can maintain collective contact. Myosin II illustrates this strategy: bipolar filaments bind oppositely oriented actin arrays and generate sliding or tension. In muscle, ordered filament geometry converts sliding into contraction. In nonmuscle cells, related contractile networks contribute to the division furrow, junction remodeling, migration and cortical tension. If the network is anchored, the same sliding mechanism can produce an approximately isometric force rather than large displacement.

Cargo transport poses a different requirement. Dimeric Myosin V motors coordinate their heads so that one remains attached while the other advances. A high-duty coordinated cycle supports myosin processivity, enabling repeated steps before dissociation. Single-fluorophore localization followed one labeled head moving by roughly twice the centre-of-mass step, supporting alternating hand-over-hand motion rather than equal short advances of both heads.^[ref] The approximate 36 nm centre-of-mass repeat reflects the actin track and motor geometry; it is not a step size shared by all myosins.

Transport and tension holding overlap. Load can slow nucleotide release and prolong strong binding, allowing some motors to act as dynamic anchors. Myosin VI can participate in endocytic membrane organization or cargo movement, depending on its partners and assembly state. Class-I myosins couple membranes to cortical actin and can regulate membrane tension and local transport. Specialized myosins organize sensory structures or long-range organelle positioning. These roles depend as much on tail-associated adaptors and local actin arrangement as on the catalytic head.

Regulation matches activity to demand. Light-chain phosphorylation can promote nonmuscle myosin II activation and filament assembly. Calcium-sensitive light chains, including calmodulin in appropriate classes, alter motor regulation or lever-arm organization. Cargo-associated adaptors can relieve autoinhibition and assemble transport complexes. Motor number, opposing loads, actin turnover and competition with other transport systems further determine the outcome.

Useful experiments separate these contributions. Actin-gliding assays establish direction and movement, single-molecule tracking measures stepping and run length, and force measurements reveal load-dependent kinetics. ATPase assays alone establish chemical turnover but not productive movement. In cells, rescue with a motor-defective or cargo-binding-defective protein can distinguish catalytic force production from a structural scaffolding role. The unifying mechanism is a coordinated affinity-and-conformation cycle; the biological output can be motion, sustained tension or controlled coupling of membranes to the cytoskeleton.

A common transition into anaphase both releases chromosomes for separation and permits the spindle to organise cytokinesis; later safeguards delay final separation when segregation remains incomplete. Temporal coordination makes the events occur in the right order, while spatial coordination positions division between the separating chromosome sets. The two forms of control interact but are experimentally distinguishable.

S phase establishes sister chromatids and their association through cohesin. During mitosis, chromosome condensation and DNA topoisomerase II activity help prepare the copies for separation. Each sister's kinetochore should attach to the opposite spindle pole, producing biorientation. Aurora B contributes to error correction by destabilising inappropriate attachments. Attachment and tension affect this process, but the spindle checkpoint should not be described simply as a direct meter of equal tension on every chromosome.

Unattached kinetochores catalyse formation of the mitotic checkpoint complex, involving Mad2, BubR1, Bub3 and Cdc20. This inhibits productive anaphase-promoting complex activity toward key substrates. In a classic causal experiment, destruction of the last unattached kinetochore allowed anaphase to proceed, with chromosome-arm damage providing an important control. It was the inhibitory signalling structure, rather than the physical presence of one unaligned chromosome somewhere in the biological cell, that maintained the delay.^[ref]

Once attachment-associated checkpoint signalling is silenced and inhibitory complexes are dismantled, anaphase-promoting complex with Cdc20 promotes ubiquitin-dependent destruction of securin and mitotic cyclin B. securin destruction permits separase activity, which cleaves the remaining cohesion-bearing kleisin subunit. Non-cleavable Scc1 blocked sister separation in budding yeast, directly linking regulated proteolysis to the loss of chromosome cohesion.^[ref] Chromosome movement can then proceed through shortening of kinetochore-associated microtubules and separation of the spindle poles.

Destruction of cyclin B also lowers CDK1 activity. This changes the phosphorylation balance, allowing protein phosphatases to reverse mitotic modifications and permitting chromosome decondensation, nuclear reassembly and cytokinetic organisation. Thus regulated proteolysis produces two coordinated outputs: removal of a physical chromosome linkage and removal of the mitotic kinase state. Their sharing of a controller improves ordering, but it does not mean that cytokinesis physically waits for a sensor to count every chromosome at its destination.

For animal cytokinesis, overlapping microtubules of the central spindle and signals associated with astral microtubules specify an equatorial cortical region. centralspindlin recruits and regulates the guanine-nucleotide exchange factor ECT2, which promotes local RhoA activation. RhoA stimulates actin assembly and myosin II activity, organising the actomyosin ring that drives furrow ingression. This geometry aligns the division plane between the segregating chromosome masses. Spindle position can itself be set by cortical cell polarity cues, explaining how the same machinery supports either approximately symmetric or asymmetric division.

Depletion and localisation experiments distinguish the biochemical signal from a simple structural scaffold. Experiments in human biological cells showed that ECT2 is required for cortical RhoA and furrow assembly, and that different centralspindlin subunits have distinguishable consequences for these events. Loss of central-spindle localisation need not abolish every equatorial signal, because additional spatial inputs can persist.^[ref] Accordingly, central-spindle disruption should be assessed alongside astral signals, spindle orientation and direct measurements of the cortical activity zone.

Furrow ingression leaves an intercellular bridge with a midbody. Final abscission involves ESCRT-III-dependent membrane-remodelling machinery and must be distinguished from the earlier contractile event. Chromatin trapped in the bridge can sustain Aurora B-dependent signalling and delay abscission. Human-cell experiments connected persistent chromosome bridges with continued kinase activity and delayed final separation, reducing the risk of unsuccessful division and furrow regression.^[ref] This safeguard can provide time to resolve a problem; persistent bridges can still lead to breakage, regression or abnormal descendants.

A decisive experimental series would image labelled chromosomes, microtubules, cyclin B, active RhoA and the biological cell boundary in the same biological cells. Acute checkpoint inhibition predicts premature anaphase and increased segregation errors. Stabilised securin or cleavage-resistant cohesion should obstruct separation; persistent cyclin B should obstruct normal mitotic exit. Acute ECT2 loss can impair cytokinesis even when chromosome segregation proceeds, demonstrating separable downstream machinery. Use timed interventions after spindle assembly, independent depletion reagents, appropriately expressed rescue constructs and controls for global biological cell damage. Count chromosome allocation, furrow initiation, ingression and abscission separately; a binucleate endpoint does not reveal which step failed.

The checkpoint also has blind spots. A merotelic attachment, where one kinetochore binds microtubules from both poles, may evade an unattached-kinetochore signal and generate a lagging chromosome. Coordination is therefore layered rather than absolute: attachment surveillance, a shared proteolytic transition, spindle-directed cortical signalling and a late abscission checkpoint jointly reduce the chance of partitioning the genome incorrectly. The detailed geometry differs in organisms that divide with a cell plate or other cytokinetic mechanisms.

A skeletal-muscle fibre contains parallel myofibrils assembled from repeating sarcomeres between Z discs. Thin actin filaments extend from the Z discs; bipolar thick myosin II filaments occupy the central region. Overlap between them allows many myosin heads to interact with actin in parallel.

A rise in cytosolic calcium exposes actin binding sites through the troponin–tropomyosin regulatory system. ATP binding releases a strongly attached myosin head; hydrolysis primes its lever arm, attachment and product release permit a force-generating stroke, and another ATP allows detachment. The cycle converts chemical free energy into mechanical work rather than consuming actin or shortening the filaments themselves.

Relative filament sliding draws the Z discs together. The I band and H zone shorten as overlap increases, whereas the thick-filament A-band length is approximately unchanged. Calcium removal restores inhibition and permits relaxation. The many-head ensemble sustains force even though individual cross-bridges repeatedly attach and detach. This sliding-filament description concerns myosin II in muscle; the processive two-head walking of Myosin V in a is a related but distinct motor arrangement.

Polarity proteins generate tissue form by controlling where cells build surfaces, place junctions and divide. Their morphogenetic roles can be separated experimentally from a wholesale loss of epithelial identity. Three examples illustrate different outputs: positioning a single lumen, orienting neighbour exchange, and limiting tube dimensions.

The first example is Cdc42-dependent lumen formation in three-dimensional Caco-2 epithelial cysts. Cells in a normal cyst coordinate their apical-basal polarity so that apical surfaces face one central lumen. During growth, a correctly oriented spindle apparatus places daughter cells into the epithelial wall rather than establishing inappropriate internal cell arrangements. Cdc42 depletion disrupts spindle orientation and produces abnormal, often multiple, luminal spaces. Importantly, the cells can still establish apical membrane identity: in this model the crucial defect is the coordination and positioning of apical surfaces during division, rather than an absolute inability to make any apical surface. This distinguishes tissue-level organization from polarity within an isolated cell.^[ref]

Mechanistically, Cdc42 connects cortical organization to the PAR polarity complex, polarized trafficking and spindle-positioning machinery. However, the relative contributions depend on the model: a Cdc42 trafficking phenotype in another epithelial line cannot simply be substituted for the Caco-2 spindle result. A convincing test combines live-cell imaging of division and the first ectopic lumen with apical and basal markers, verifies target depletion and rescues with functional Cdc42. Compare the total number and viability of cells, because a dying cell population can also produce abnormal cavities. A perturbation that restores spindle positioning while leaving other outputs of Cdc42 impaired would help isolate the causal route. These controls make the single-lumen phenotype an interpretable morphogenetic output.

The second example is Bazooka, the fly PAR-3 protein, during Drosophila germband extension. This uses planar cell polarity within the epithelial sheet as well as apical-basal organization. Bazooka and junctional components become enriched at a complementary set of cell interfaces to myosin II. Spatially patterned gene activity organizes this planar asymmetry, and loss of Bazooka disrupts normal polarized cell behaviour and extension. Thus a protein associated with epithelial junction assembly is redeployed to make different junctions behave differently in the same sheet.^[ref]

Oriented junction shrinkage and new-junction formation permit cell intercalation while maintaining epithelial continuity. The important geometry is that junctions separating anterior and posterior neighbours shrink and resolve into interfaces with the complementary orientation, producing extension along the body axis. Junction names can be confusing because they may describe either the neighbours or the line itself; tracking vertices and neighbour exchange avoids this ambiguity. Bazooka is a spatial organizer, not itself the force-generating motor. To test its contribution, quantify its localization, myosin localization, junction lifetimes, cell rearrangements and tissue strain after an acute or mosaic perturbation that leaves enough epithelial structure for movement to occur. A general epithelial collapse would establish an essential structural role but would not isolate its role in planar coordination.

The third example is control of fly tracheal tube size by the apical determinant Crumbs and basolateral regulators including Yurt and Coracle. Crumbs promotes the apical domain, so restricting its activity helps constrain the amount of luminal cell surface and hence tube dimensions. Mutations in yurt produce overlong tracheal tubes, and reducing Crumbs dosage suppresses important length defects; Crumbs overexpression has the opposite tendency. This genetic interaction connects the balance of apical and basolateral regulators to organ geometry rather than simply to the presence of an epithelial sheet.^[ref]

The luminal extracellular matrix is a crucial control in this example. Septate-junction-associated proteins can also affect delivery of the matrix-modifying protein Vermiform, potentially changing tube shape indirectly. Yet yurt mutants retain Vermiform secretion, and reducing Crumbs can suppress coracle length defects without restoring the secretion defect. Scribble mutants also show long tubes but are not equivalently rescued by the tested Crumbs reduction. The result supports parallel and partly distinct routes, rather than a universal linear pathway in which every basolateral protein merely inhibits Crumbs. Compare cell number, apical area, tube length and diameter independently: a longer tube need not result from extra divisions. Quantitative dosage interactions and rescue are particularly informative because they can reveal a size-control function while preserving much of epithelial organization.

Together, these examples link polarity to three separable operations. Cdc42 coordinates the location of new apical surfaces during division; Bazooka contributes to directional junction remodelling within a sheet; and the Crumbs-regulator balance sets the extent of a luminal surface. Conversely, changing forces and geometry can alter junctional organization, so the relationship is reciprocal. The common principle is that epithelial polarity supplies spatial constraints on growth and rearrangement. It is a dynamic component of morphogenesis, not merely a static property to be established before morphogenesis starts.

Mechanics shapes tissues by generating active forces, directing rearrangements and converting constrained growth into deformation. Three experimentally distinct examples are folding of the fly ventral epithelium, elongation of the fly germband and formation of chick intestinal villi. They respectively emphasize changes in cell shape, changes in cell neighbours and a growth-driven instability. In each case, a satisfactory explanation needs both a force-generating process and the material or boundary conditions that convert it into a particular shape.

First, apical constriction drives Drosophila ventral furrow formation. Ventral cells accumulate a contractile actomyosin network near their apical surfaces. Reducing apical area while retaining tissue continuity changes cell geometry and contributes to inward bending of the epithelial sheet. This is not adequately described as uniform contraction of a permanent circumferential belt. Time-resolved imaging showed pulses of medioapical myosin II accumulation associated with discrete contractions, and stabilization between pulses permits net constriction. Regulation by Snail and Twist helps coordinate contraction and the retention of the resulting shape.^[ref]

The force must be transmitted to neighbouring cells through adherens junctions; a detached contracting cortex can deform internally without folding a coherent sheet. Geometry is therefore a collective property. A useful causal test compares acute inhibition of myosin activation with perturbation of junctional coupling, scoring apical area, contraction pulses, cell length and tissue curvature separately. laser ablation can reveal the direction of tissue load, and localized activation of contractility can test whether the site of force generation predicts bending. Recoil velocity alone is not tension: in an overdamped approximation $v_0\sim T/\zeta$, where $T$ is released tension and $\zeta$ an effective resistance. Comparing recoil between conditions requires considering possible changes in resistance as well as load. External pressure, basal constraints and neighbouring tissue movement also influence invagination, so apical contraction need not be sufficient under every boundary condition.

Second, Drosophila germband extension changes tissue aspect ratio through oriented cell intercalation. Selected cell junctions shrink, cells briefly share a vertex or multicellular rosette, and new junctions appear in the complementary orientation. Repeated local neighbour exchanges extend the tissue along one axis while narrowing it along the other. myosin II is enriched at the shrinking interfaces, and interfering with its activity disrupts polarized junction remodelling. This supplies a mechanism for convergent extension without requiring that every cell grow longer or that an increased number of divisions provide the extension.^[ref]

Here the crucial distinction is between active rearrangement and passive stretching. Track all vertices and neighbours in a patch and decompose tissue deformation into cell-shape change, neighbour exchange and cell-number change. A tissue can lengthen while individual cells remain similar in shape if topology changes; alternatively, pulling from a neighbouring tissue can elongate cells without local intercalation supplying the force. Test whether local myosin inhibition suppresses the junction transitions before global tissue movement is lost, and compare spatial patterns of load by laser ablation. Rescue must restore directional transitions as well as the final length. planar cell polarity provides the orientation, and junctional adhesion permits force transmission while contacts are remodelled. Thus mechanics can translate a molecular anisotropy into coordinated movement of an epithelial sheet.

Third, chick intestinal villi illustrate differential growth constrained by surrounding layers. The growing inner tissues are enclosed by sequentially differentiating smooth muscle layers. Mechanical constraints drive a progression from longitudinal ridges through zigzags toward a villous surface. The important process is not simply muscle contraction pushing each villus into place: the muscle acts as a restricting layer against which continued tissue growth builds compressive stress. In the primary experiments, blocking muscle differentiation prevented the expected folding, while an artificial constraining silk tube could restore folding in the inhibited tissue. This rescue is particularly informative because it replaces a living layer's mechanical contribution without restoring all its possible signals.^[ref]

The physical principle is a buckling instability: a sufficiently compressed growing layer can lower its mechanical cost by bending. The wavelength and mode depend on geometry, thickness and stiffness, so equal amounts of growth need not yield equal shapes in different environments. An ideal thin-plate model has bending rigidity $B=E{h}^3/[12(1-{\nu }^2)]$, with Young's modulus $E$, thickness $h$ and Poisson's ratio $\nu$. It predicts strong thickness sensitivity of resistance to bending, but this formula alone does not compute the wavelength of a living multilayer gut. That requires measured geometry, growth and an appropriate constitutive model. Compare proliferation, muscle differentiation, material properties and folding after each perturbation to distinguish mechanical confinement from secondary effects on growth.

The chick example should not be imposed unmodified on mouse villus development, where mesenchymal cluster patterning precedes the corresponding epithelial deformation. Nor is any of the three mechanisms independent of chemical signalling: signals position contractility, specify muscle and regulate adhesion, while mechanical deformation changes the subsequent signalling environment. Their distinct causal signatures are nonetheless clear. A contractile apical network folds a coupled sheet; anisotropic junctional tension changes neighbours and tissue aspect ratio; constrained growth generates an instability whose form depends on material properties. Testing these signatures through timed perturbation and mechanical rescue explains organ shape more precisely than simply observing that a cytoskeletal protein is required.