| Literature DB >> 35573681 |
Dagmar Iber1,2, Malte Mederacke1,2.
Abstract
The trachea is a long tube that enables air passage between the larynx and the bronchi. C-shaped cartilage rings on the ventral side stabilise the structure. On its esophagus-facing dorsal side, deformable smooth muscle facilitates the passage of food in the esophagus. While the symmetry break along the dorsal-ventral axis is well understood, the molecular mechanism that results in the periodic Sox9 expression pattern that translates into the cartilage rings has remained elusive. Here, we review the molecular regulatory interactions that have been elucidated, and discuss possible patterning mechanisms. Understanding the principles of self-organisation is important, both to define biomedical interventions and to enable tissue engineering.Entities:
Keywords: SOX9; Turing pattern; cartilage rings; chemotaxis; differential adhesion; differential growth; symmetry break; trachea
Year: 2022 PMID: 35573681 PMCID: PMC9094403 DOI: 10.3389/fcell.2022.900447
Source DB: PubMed Journal: Front Cell Dev Biol ISSN: 2296-634X
FIGURE 1Tracheal cartilage ring formation. (A) Cartilage rings (red) emerge in the mesenchyme on the ventral (V) side of the trachea. (B) Cross-section of the developing trachea. (C) Regulatory interactions that control the emergence of cartilage rings (CR) in the ventral and airway smooth muscle in the dorsal (D) tracheal mesenchyme. Black arrows indicate positive regulation, red arrows negative regulation. For details see text.
FIGURE 2(A) Repetitive patterns can emerge via a Turing mechanism when two regulatory factors that diffuse at different speeds engage in a negative feedback Turing (1952). In case of the ligand-receptor based Turing mechanism, the binding of the rapidly diffusing ligand (L) to the slowly diffusing receptor (R) results in up-regulation of the receptor and removal of the ligand. This system can be modelled with two coupled partial differential reaction diffusion equations. This system can yield a large variety of patterns, dependent on the reaction parameters and the tissue geometry. (B) Chemotaxis can result in periodic patterning when motile cells (C) produce and consume the diffusible chemoattractant or chemorepellent (L), as modelled for instance by the Keller-Segel model Keller and Segel (1971). (C) Differential adhesion between the blue and the red cells can result in periodic pattern formation. The mixture of cells is dependent on their relative surface tension (CT1 for the red, CT2 for the blue population). This results in three different relative surface tensions (T1 between red cells, T2 between blue and T12 between the two populations) Canty et al. (2017). To achieve separation in the displayed form CT1 must be larger than CT2 and T1 larger than T12 which is larger than T2. (D) Differential growth of two adjacent tissue layers can result in buckling. The wavelength λ of the periodic pattern depends on the thickness, h, of the expanding epithelial layer (blue layer), and the relative Young modulus E /E of epithelium (blue) and mesenchyme (red) Sultan and Boudaoud (2008).