Past exam of the zoology course of the University of Cambridge / 2025 / Paper zl6 / 6

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.