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Modelling of morphogenesis to support the design of fungal-based engineered living materials

Published online by Cambridge University Press:  30 September 2024

A response to the following question: How do we design with materials that have their own agency?

Vilhelm Carlström*
Affiliation:
Chair for Biohybrid Architecture, Royal Danish Academy, Copenhagen, Denmark
Adrien Rigobello
Affiliation:
Chair for Biohybrid Architecture, Royal Danish Academy, Copenhagen, Denmark
Phil Ayres
Affiliation:
Chair for Biohybrid Architecture, Royal Danish Academy, Copenhagen, Denmark
*
Corresponding author: Vilhelm Carlström; Email: cham@kglakademi.dk
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Abstract

To realize the potential of materials comprising living organisms, bioengineers require a holistic understanding of the reciprocal relationship between environmental conditions and the biochemical and biophysical processes that influence development and behaviour. Mathematical modelling has a critical part to play in managing the complexity of biological dynamical systems and attaining higher degrees of control over their trajectories and endpoints. To support the development of mycelium-based engineered living materials, this paper reviews the literature of growth models for filamentous fungi with emphasis on the connection between morphogenesis and metabolism.

Information

Type
Analysis
Creative Commons
Creative Common License - CCCreative Common License - BYCreative Common License - NCCreative Common License - SA
This is an Open Access article, distributed under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike licence (https://creativecommons.org/licenses/by-nc-sa/4.0/), which permits non-commercial re-use, distribution, and reproduction in any medium, provided the same Creative Commons licence is used to distribute the re-used or adapted article and the original article is properly cited. The written permission of Cambridge University Press must be obtained prior to any commercial use.
Copyright
© The Author(s), 2024. Published by Cambridge University Press
Figure 0

Table 1. Overview of fungal morphogenesis models from the literature

Figure 1

Table 2. Overview of fungal morphogenesis models from the literature

Figure 2

Figure 1. Pure mycelium sheet of Ganoderma lucidum grown on beech wood imaged at various magnifications. The properties of the macroscopic material depend on the microscopic structure. The salient question for modelling is how much detail needs to be represented to capture the variation in the properties of interest. a) Sheet of diameter 14 cm. The inset shows a 5 mm square slice on microscope stage with cross-hairs marking position of focus. b) Material imaged at 630x magnification, cropped to a 500 $\mu $m square. c) Material imaged at 6300x magnification, cropped to a 50 $\mu $m square.

Figure 3

Figure 2. Example output of a generic lattice-free discrete-continuum hybrid model in a 2D domain. a) A discrete hyphal network generated as trails left by agents propagating by lateral branching and a random walk biased by a chemical gradient in the external environment. Each hypha is generally represented as an array of the coordinate visited in each iteration. One of the advantages of discrete representation is that it allows for topological network analysis. b) A continuous chemical concentration caused by secretion from the tips and subsequent diffusion in the medium, resulting in a smooth gradient. The evolution of the chemical concentration is calculated with a PDE, in which the dynamics are consistent with physical phenomena.

Figure 4

Figure 3. Examples of Monod-type functions. a) For a single variable a Monod equation is typically parameterized by a maximum reaction rate, ${{\rm{\mu }}_{max}}$, that the function approaches asymptotically, and a Michaelis constant, ${K_m}$, which is the concentration at which the reaction rate reaches half of the maximum. As the concentration goes to zero the slope approaches ${{\rm{\mu }}_{max}}/{K_m}$. Additional control can be achieved by modifying the function. In the example, the function is shifted by a threshold, $t$, below which the reaction rate is zero, and changing the sign makes the effect of increasing concentration inhibitory (blue). Monod-like functions can be useful for describing simple systems because the parameters are few, but capture important information about the overall behaviour of the system. In reality, an organism’s reliance on any single variable is more complicated. For example, excessively high concentrations of useful compounds may be toxic, and while temperature increases the rate of chemical reactions generally, this also implies increasing maintenance costs. b) For multiple variables a straightforward approach is to use the product of a Monod-like expression for each variable, each with its own set of parameters. Metabolic behaviour is nonlinear and there is, of course, no guarantee that the interaction between variables is multiplicative, but it can serve as a simple descriptive model. While the properties of the resulting system are similar to the one-dimensional case it is important to consider that the asymptotic approach to the maximum rate becomes much slower, and the meaning of the Michaelis constant must be regarded in relation to the other variables. In a two-variable system, if both concentrations are at the level of their respective Michaelis constant, the reaction rate is one fourth of the maximum rate rather than half.

Figure 5

Figure 4. Transport mechanisms reported in fungi. The diagrams are read as a before and after state from left to right. a) Diffusion is one of the mechanisms by which particles are transported both within the mycelium and in the external substrate. The large number of particles and stochasticity involved, along with the fineness of the process compared to the scale of hypha, means it is usually represented as a continuous process. Diffusion can be represented as one-dimensional (longitudinal) between segments of discretized hypha. b) Vesicular transport, is the advection of particles gathered in vesicles within the hypha and drawn by molecular motors walking (unidirectionally) along cytoskeletal filaments. The moving vesicles can cause cytoplasmic streaming which drags smaller external molecules along with them. c) Hydraulic transport is caused by drops in pressure potential as water is lost locally either by exudation or volume increase as the tip extends. Particles are moved by the water flowing along the pressure gradient to replace the volume lost. d) Absorption of molecules from the external environment, and secretion in the opposite direction, is usually an active process. In most models this step is simply implied and baked into a total metabolic rate, but in reality metabolic processes occur in different compartments and in series of chemical reactions. Identifying rate limiting steps in these series can be an effective way of simplifying models.

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Figure 5. Common microstructural dynamics in ABM models. The diagrams are read as a before and after state from left to right. e) Anastomosis is the fusion of a hyphal tip with another hypha. Algorithmically this generally requires collision detection which is relatively computationally involved. Since the exact position of the hypha may be difficult to determine, and as the conditions required for anastomosis to occur may be unknown, the event is often simply assumed to have occurred with some probability when tips come within an arbitrary distance of other hypha (for example within the same cell of a simulation lattice). A collision angle may also be used to determine the likelihood of the event. f) Apical branching is relatively simple to represent as a hyphal tip simply becomes two tips, parameterized by a change in direction. A function of internal and/or external conditions determines the frequency of branching events—in the simplest case stochastic events can be drawn from a cumulative probability distribution with the desired properties (mean, std. deviation). It may be useful to consider that branching at a well-defined rate is equivalent to exponential growth in a continuum regime. g) Sub-apical or lateral branching is more subtle because the algorithm also needs to consider how far behind the tip and how far in front of the last branch new branches should appear. This can complicate the procedure by necessitating additional length calculations and the storage of more microstructural data. h) Random-walk is the most common way of representing tip propagation. At each iteration the position of the tip is updated by a propagation speed given by some function, and a new direction drawn from some probability distribution. If the update velocity is not uniformly distributed over the circle (2D) or sphere (3D) of possible directions the random walk is said to be biased, which can be used to represent various tropisms. For example, in chemotaxis the presence or absence of an external substance may bias the distribution of update velocities, causing growth away from or towards the substance concentration gradient. Notably, taking the continuum limit of randomly walking agents, or the expected value of displacement, is equivalent to diffusion.

Figure 7

Figure 6. Some tropisms reported in fungi. i) Chemotropism is where the direction of hyphal extension is either attracted or repelled by a chemical gradient. In so far as secretion and depletion of substrate compounds create such gradients, chemotropism could provide signals that allow hyphae to navigate towards or away from each other, autotropism. j) Gravitropism can be observed where hypha extend away from the substrate surface as in aerial hypha, directed by the gravity vector. k) Galvanotropism lets hypha reorient in response to electric fields. It is perhaps not a naturally occurring phenomena, but an effect of the role of ions in the general navigation mechanism. l) Thigmotropism is where hypha appear to follow geometrical features like ridges or grooves in the environment and is mediated by pressure or stretch sensing. Thigmotropism may play a role where fungi navigate structured substrates like wood, and where hypha bundle together with other hypha, providing another instance of autotropism.