Abstract
This chapter uses continuum theories for growth and contraction to simulate morphogenesis in embryos. First, the cellular activities underlying tissue-scale morphogenesis are discussed. Next, to illustrate basic concepts in epithelial morphogenesis, a linear theory for growing beams and plates is presented and used to solve illustrative examples involving some basic morphogenetic processes. The full nonlinear theory is then used to solve problems in embryonic development, including gastrulation, neurulation, and organogenesis. Examples of organogenesis include the development of the early heart and brain, the eyes, the gut, and the lung. A buckling analysis is used to simulate folding of the cerebral cortex. Finally, mechanical feedback and a theory for mesenchymal morphogenesis are discussed.
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Notes
- 1.
Technically, stretching involves deformation caused by stress. For convenience, as used here, the term also includes dimensional changes that do not involve true deformation, such as growth that does not generate stress.
- 2.
The linear theory also offers opportunities for creating homework and exam problems.
- 3.
- 4.
It is a simple matter to enforce incompressibility of fiber volume during contraction, i.e., set \(\det \mathbf {G}=1\). For simplicity, however, this constraint is sometimes ignored in this chapter.
- 5.
This expression represents an approximation to the exact relation κ = (dθ∕dx)∕(1 + θ 2)3∕2 for θ 2 << 1.
- 6.
These boundary conditions are analogous to specifying either displacement or force for a traditional spring and either rotation angle or moment for a torsional spring.
- 7.
For convenience, although the force and moment resultants are defined differently, their symbols are kept the same.
- 8.
Some readers may want to verify this result for themselves.
- 9.
To compare results with the “exact” solution, try Problem 8.5.
- 10.
- 11.
The HT is relatively transparent at these stages.
- 12.
In Fig. 8.39, tissue labels injected along the ventral midline of the HH10 HT move toward the right or left edge in ventral view.
- 13.
As new information becomes available, developmental biologists sometimes change their terminology. Recently, the forebrain has been described as dividing into the diencephalon and secondary prosencephalon (Fig. 8.42, HH20). The secondary prosencephalon includes the optic vesicles, the hypothalamus, and the telencephalon.
- 14.
The bar may eventually stop rotating at some rotation angle, which can be computed using a nonlinear analysis for large rotation (see Problem 8.7).
- 15.
For p≠0 or M g≠0, the beam bends without buckling.
- 16.
In general, for a differential equation of order n, boundary conditions should involve derivatives no higher than n − 1.
- 17.
- 18.
The study of Shyer et al. (2013) represents an outstanding example of how clever experiments, computational models, and physical models can be integrated to solve a challenging problem in the mechanics of morphogenesis. It is highly recommended to all readers of this book.
- 19.
- 20.
Similarly, to obtain realistic growth in a developing artery, we earlier assumed that the target stresses increase with blood pressure [see Eq. (6.128)].
- 21.
Tissue contraction is not always of the actomyosin variety. It also could occur, for example, by cell death (apoptosis), outward cell migration, or resorption of cell membranes.
- 22.
For simplicity, contraction is not treated as an isovolumic process in this problem.
- 23.
In this problem, the wall expands by radial intercalation, with deeper cells moving between those above. This process causes the wall to spread and become thinner.
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Taber, L.A. (2020). Morphogenesis. In: Continuum Modeling in Mechanobiology. Springer, Cham. https://doi.org/10.1007/978-3-030-43209-6_8
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