Abstract
Since the discovery of cells by Robert Hooke and Antoni van Leeuwenhoek in the 17th century, thousands of different cell types have been identified, most recently by sequencing-based single-cell profiling techniques. Yet, for many organisms we still do not know, how many different cell types they are precisely composed of. A recent survey of experimental data, using mostly morphology as a proxy for cell type, revealed allometric scaling of cell type diversity with organism size. Here, I argue from an evolutionary fitness perspective and suggest that three simple assumptions can explain the observed scaling: Evolving a new cell type has, 1. a fitness cost that increases with organism size, 2. a fitness benefit that also increases with organism size but 3. diminishes exponentially with the number of existing cell types. I will show that these assumptions result in a quantitative model that fits the observed cell type numbers across organisms of all size and explains why we should not expect isometric scaling.
Introduction
Since the advent of high throughput single-cell profiling techniques, a large number of cell types has been catalogued across many different tissues. For example, the Tabula Sapiens consortium recently identified over 400 cell types across 24 different human tissues (). Whether each cluster of transcriptomes or other molecular profiles should be considered a separate cell type is still under debate (; ) and we certainly need improved methods to discriminate biologically meaningful variability from random noise (). Nevertheless, single-cell profiling has revealed a high diversity of cell states and one might be forgiven to wonder: Could each cell be its own, highly specialized cell type? Here, I will argue, from an evolutionary fitness perspective, that we should expect much fewer cell types than cells in an organism. Whole-organism single-cell transcriptomics data sets are currently still rare () and, as mentioned above, uncertainties in the interpretation of these data sets remain. To circumvent these problems, I base my arguments on recent studies by Fisher et al. (; ), who collected published cell type numbers, mostly derived from morphological characteristics. These studies found that the number of cell types scales allometrically with the total number of cells in the organism (Figure 1). Intriguingly, the data could not be fit by a single power law, in contrast to many other allometric relationships (). As shown in seminal work by Geoffrey West and co-workers, power law scaling can arise from the optimization of metabolic rate subject to geometric constraints of relevant tissues, such as the vasculature (; ; ; ). Fisher et al. therefore fit two separate power laws, for small and large organisms, respectively, suggesting that larger organisms face additional constraints. In contrast to the allometric scaling of metabolic rate, it is not immediately obvious that geometric or physiological constraints should be the only relevant factors for cell type allometry. One might therefore not expect a priori to find power law scaling.
FIGURE 1
Diminishing returns model
Here, I develop an alternative model that can explain the observed scaling across organisms of all sizes. This model considers the effect of a new cell type on an organism’s fitness. I adopt a notion of fitness described by Wagner as “a measure predicting the competitive ability of a genotype compared to another” (
Requiring for a new cell type to appear leads to
To rigorously compare this ‘diminishing returns’ model with the double power law, I used a Bayesian hierarchical approach (see Materials and Methods for the model definitions and priors). I assumed that the cell type numbers are normally distributed in log-space with a mean given by the double power law (i.e., a piecewise linear relationship in log-space) or the relationship derived above. Initially, I assumed the standard deviation to be constant (Figure 1, left column). Posterior distributions of the parameters were obtained by Markov Chain Monte Carlo sampling. Estimates of the slopes and breakpoint in the double power law were very similar to those obtained by Fisher et al. (
TABLE 1
| Fisher et al. | Double power law, constant sd | Diminishing returns, constant sd | Double power law, variable sd | Diminishing returns, variable sd | |
|---|---|---|---|---|---|
| intercept k0 [HDI] | −0.20 [−0.41,−0.01] | −0.19 [−0.30,−0.08] | |||
| slope (small N) ssmall [CI or HDI] | 0.21 [0.16,0.26] | 0.21 [0.14,0.29] | 0.20 [0.16,0.25] | ||
| breakpoint nbp [CI or HDI] | 4.80 [3.90 5.70] | 4.82 [2.81,6.64] | 5.18 [3.52,6.84] | ||
| slope (large N) slarge [CI or HDI] | 0.07 [0.03 0.11] | 0.07 [0.03,0.10] | 0.06 [0.01,0.10] | ||
| A [HDI] | −0.29 [−0.64,0.08] | −0.13 [−0.42,0.16] | |||
| B [HDI] | 1.29 [1.09,1.49] | 1.13 [0.94,1.33] | |||
| sd Σ [HDI] | 0.32 [0.29 0.36] | 0.33 [0.29,0.37] | |||
| sd intercept Σ0 [HDI] | 0.12 [0.06,0.19] | 0.17 [0.10,0.24] | |||
| sd slope sΣ [HDI] | 0.03 [0.02,0.04] | 0.02 [0.01,0.04] | |||
| elpd [se] | −39.96 [7.74] | −43.22 [8.08] | −28.25 [8.97] | −35.52 [7.82] |
Estimates of model parameters and model comparison. The power law parameters reported by
Discussion
In the derivation presented here, I made several assumptions that require critical assessment. First, I implied that cell types are discrete and stable entities, while others put forward the notion of dynamic cell states that lie on a continuum (
In summary, I developed a phenomenological model of cell type allometry using a minimal number of assumptions. The model is therefore agnostic of evolutionary lineages and related systematic differences. Nevertheless, I showed that diminishing fitness benefits can explain the observed cell type allometry. I hope that this manuscript will stimulate experiments and the development of more sophisticated models.
Materials and methods
The experimental data shown in Figure 1 was published previously (
To compare the double power law model with the ‘diminishing returns’ model, a Bayesian hierarchical approach was used. The log-cell type number k was assumed to be normally distributed. For the double power law, the mean of the normal distribution is given by a piecewise linear relationship between n and k. In the case of constant standard deviation (i.e., the spread of k does not depend on the log-cell number n), the double power law model is thus defined bywhere k0 is the intercept of log-cell type numbers k, and ssmall and slarge are the slopes below and above the breakpoint nbp, respectively. Normal indicates a normal distribution with mean μ and standard deviation σ, Uniform is a uniform distribution between a and b, and HalfCauchy is a Cauchy distribution at location 0 with half-width half-maximum γ that was truncated below 0 so that only positive values have non-zero probability.
For variable standard deviation (i.e., the spread of the log-cell type number k increases linearly with log-cell number n) the model is defined bywhere Σ0 and sΣ are the intercept and slope, respectively, of the linear model for the standard deviation. HalfNormal is a Normal distribution with mean μ = 0 and standard-deviation σ truncated below 0 such that only positive values have non-zero probabilities.
The ‘diminishing returns’ model, which assumes the fitness benefit to decrease with cell type number, is correspondingly defined by
in the case of constant standard deviation and by
when the standard deviation is allowed to increase linearly with log-cell number n.
The posterior distributions of all parameters were obtained by Markov Chain Monte Carlo sampling using the python package pymc (version 4.1.2) with 2 chains, 2000 tuning steps and 10,000 samples. The “target_accept” parameter was kept at the default value of 0.8 except for the ‘diminishing returns’ model with constant standard deviation. That model required a “target_accept” of 0.99 to avoid divergences. For model comparison, the arviz python package (version 0.12.1) was used to estimate the expected log posterior density (elpd) by leave-one-out cross-validation. The regression curves shown as solid lines in Figure 1 are posterior means of f(n): For each n, the average of f(n) over the posterior distribution of the parameters was calculated. The 95% highest density intervals (HDIs) shown as blue bands in Figure 1 correspond to the smallest intervals that contain 95% of the posterior distribution of f(n) for a specific n. The 95% HDIs of the posterior predictive distribution (ppd) correspond to the smallest intervals containing 95% of the posterior distribution of the log-cell type number k for a given n.
The jupyter notebook used to produce all presented results from the raw data can be obtained from github (https://github.com/semraulab/allometry).
Statements
Data availability statement
The dataset used in this study is publicly available from Dryad under a CC0 Universal (CC0 1.0) Public Domain Dedication license: https://datadryad.org/stash/dataset/doi:10.5061/dryad.27q59.
Author contributions
SS conceived of the model, carried out the data analysis and wrote the manuscript.
Acknowledgments
I am very grateful to Itai Yanai, Liedewij Laan, and Günter Wagner for encouragement, discussions and comments on the manuscript. I would like to thank Maria Mircea for proofreading the manuscript.
Conflict of interest
The author declares that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Publisher’s note
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.
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Summary
Keywords
single-cell omics, cell type, allometry, power law, evolutionary fitness
Citation
Semrau S (2022) Why isn’t each cell its own cell type? Diminishing returns of increasing cell type diversity can explain cell type allometry. Front. Cell Dev. Biol. 10:971721. doi: 10.3389/fcell.2022.971721
Received
17 June 2022
Accepted
19 August 2022
Published
10 October 2022
Volume
10 - 2022
Edited by
James J. Cai, Texas A&M University, United States
Reviewed by
Arti Ahluwalia, University of Pisa, Italy
Adrianus J. Westgeest, CEFE, France
Jiri Neustupa, Charles University, Czechia
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© 2022 Semrau.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Stefan Semrau, semrau@physics.leidenuniv.nl
This article was submitted to Evolutionary Developmental Biology, a section of the journal Frontiers in Cell and Developmental Biology
Disclaimer
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article or claim that may be made by its manufacturer is not guaranteed or endorsed by the publisher.