Abstract
10
Understanding human cell metabolism through genome -scale flux profiling is of interest to diverse 11
research areas of human health and disease. Metabolic modeling using genome -scale metabolic 12
models (GEMs) has the potential to achieve this, but has been limited by a lack of appropriate input 13
data as model constraints. Here we show that GEM-based flux profiling simulations can be improved 14
with an appropriate input data collection procedure and exo -metabolite exchange flux calculation 15
method, called regression during exponential growth phase (REGP). Our results show that the GEM-16
simulated feasible flux space is constrained to a biologically meaningful region, allowing an exploration 17
of the basic organizing principles of the feasible flux space. These improvements help to fulfil the 18
promise of GEMs as a valuable tool in the study of human metabolism and future development of 19
translational applications. 20
Keywords
21
Cell metabolism; genome-scale metabolic modeling; flux profiling; feasible flux space 22
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Introduction
23
Metabolism of human cells is a highly complex network of thousands of metabolites and reactions. 24
Alterations in cell metabolism are associated with many complex health conditions such as diabetes, 25
inflammatory diseases, and cancer (1,2). Importantly, the defining feature of metabolism is not the 26
concentrations of metabolites in the cell, but the metabolic fluxes (π) through reactions and pathways 27
(3,4). Intracellular m etabolic fluxes can be experimentally determined through isotope -labeled 28
substrate tracing for a small subset of reactions (5,6), but to systematically profile all fluxes of a cell at 29
the genome-scale, mathematical modeling is necessary. 30
Genome-scale metabolic models (GEMs) is a modeling framework wherein the complete metabolic 31
network of a cell is reconstructed in silico (5,7). GEMs can be used for simulations to calculate the 32
optimal (max or min) fluxes of each reaction, and determine the feasible flux space for the entire 33
metabolic network, using techniques called flux balance analysis (FBA) and flux variability analysis 34
(FVA) (8). FBA and FVA requires a small amount of input data as constraints, typically consisting of 35
measured exchange fluxes ( Β± measurement error) of a small number of exo -metabolites, such as 36
glucose, lactate, and amino acids. With these experimentally measured input data, GEM simulations 37
have been shown to be strikingly accurate in microorganisms such as E. coli and S. cerevisiae (9β11). 38
Critically, FBA and FVA assume that cells are in steady -state. Thus, input data for these successful 39
applications of GEM simulations have all been collected during exponential growth. 40
Building on the success of GEM simulations in microbial applications, there is considerable interest in 41
studying human cell metabolism using Human-GEM (3,12,13). The current practice to determine exo-42
metabolite exchange fluxes in human cells is to use the consumption and release (CORE) (4) method 43
(Fig 1A). In this method, exo-metabolite concentrations in the cell culture medi a are measured at a 44
single time point , and e xchange fluxes are then calculated based on the difference between the 45
measured βspentβ medi a and the unused (βfreshβ) medi a (Fig 1A) . Thus, CORE -calculated exchange 46
fluxes are not true steady-state exchange fluxes, and the use of these values as constraints for FBA and 47
FVA should be done with caution. 48
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In this study, we measured exo-metabolite concentrations at multiple time points during exponential 49
growth for a human cell line MCF10A, and calculate d exo-metabolite exchange fluxes by regression 50
during exponential growth phase (REGP ; Fig 1B ). We found that REGP-calculated exchange fluxes 51
(ππ,π
πΈπΊπ) were substantially different from CORE-calculated exchange fluxes (ππ,πΆππ
πΈ). Using ππ,π
πΈπΊπ 52
as input data for FBA and FVA, we showed that the GEM-simulated feasible flux space was constrained 53
to a more biologically meaningful region, allowing an exploration of the basic organizing principles of 54
the feasible flux space. We anticipate tha t future application of ππ,π
πΈπΊπ as input data for GEM 55
simulations can rapidly advance our understanding of cell metabolism in diverse applications related 56
to human health and disease. 57
Results
58
Exo-metabolite exchange fluxes at steady-state 59
We measured the exo-metabolite concentrations of exponentially-growing MCF10A cells at five time 60
points during the exponential growth steady-state (Supplemental Table 1), and used both the CORE 61
(Fig 1A) and REGP (Fig 1B) methods to calculate the exchange fluxes of exo-metabolites, ππ. Fig 1C 62
shows the comparison between ππ,π
πΈπΊπ and ππ,πΆππ
πΈ in the MCF10A cell lines, as well as the ππ,πΆππ
πΈ 63
of 11 cell lines of the NCI -60 panel that were previously considered reliable (3,4,14). By convention, 64
consumption of metabolites (e.g. glucose) is represented by a negative flux, and release of metabolites 65
(e.g. lactate) by a positive flux. As expected, ππ,πΆππ
πΈ were comparable between MCF10A cells and the 66
11 cell lines of the NCI-60 panel (Fig 1C). However, the ππ,π
πΈπΊπ and ππ,πΆππ
πΈ in MCF10A cells, based on 67
the same raw metabolite measurements and cell count data, were substantially different. For several 68
exo-metabolites, for example glutamate and glycine, ππ,πΆππ
πΈ values were positive, indicating that cells 69
were releasing these metabolites into the culture media; while ππ,π
πΈπΊπ values were negative, 70
indicating that cells were consuming these metabolites as nutrients. As the CORE method 71
encompasses both lag phase and exponential growth phase (Fig 1A) , whereas the REGP method 72
calculates the exchange flux during exponential growth only (Fig 1B), this reflects that cell metabolism 73
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differs between lag phase and exponential growth (Fig 2). Our results indicate that glutamate is 74
released by the cells during lag phase, and consumed during exponential growth (Fig 2B). Similarly, 75
consumption of glycine differs between lag phase and exponential growth (Fig 2C). 76
For other nutrients, such as glucose, glutamine, and other amino acids, i n general we observed that 77
ππ,π
πΈπΊπ for nutrient consumption were larger (that is, more negative) than ππ,π
πΈπΊπ, consistent with a 78
higher nutrient consumption rate during exponential growth compared to the lag phase (Fig 1C). For 79
the metabolic waste lactate, we observed that the exchange flux for lactate release was smaller (that 80
is, less positive) by the REGP method (Fig 1C), suggesting that lactate production is elevated during the 81
lag phase, and reduced during exponential growth. 82
Simulating steady-state cell growth 83
A common way to benchmark FBA- and FVA-based GEM simulations is to estimate the cell growth rate 84
(3,15), which can be easily validated experimentally. To do this, we first constructed cell line-specific 85
GEMs by tINIT (16) using cell-line specific transcriptomics data, generated in-house for MCF10A cells 86
(Supplemental Table 2; GEO accession GSE293588) and mined from the Cancer Cell Line Encyclopedia 87
(17) for the 11 cell lines of the NCI-60 panel. We then specified the metabolites that are present in the 88
cell culture media (Hamβs medium), followed by constraining the exo-metabolite exchange fluxes (Fig 89
1C). For MCF10As, either ππ,πΆππ
πΈ or ππ,π
πΈπΊπ were used; for the 11 cell lines of the NCI-60 panel, only 90
the available ππ,πΆππ
πΈ were used (see Fig 3). Based on these input data as model constraints, the range 91
of feasible in silico growth rates were simulated by maximizing and minimizing biomass production. 92
We found that the ππ,πΆππ
πΈ-constrained MCF10A model was infeasible (Fig 3A), meaning that the in 93
silico cell was unable to βgrowβ with the CORE -calculated metabolite uptake and secretion rates. In 94
contrast, the ππ,π
πΈπΊπ-constrained MCF10A model was feasible (Fig 3A). Critically, the experimentally 95
measured growth rate fell within the GEM-simulated solution space (Fig 3A) , indicating that GEM -96
simulations are physiologically relevant when using ππ,π
πΈπΊπ as constraints, but not with ππ,πΆππ
πΈ. 97
Similar to the ππ,πΆππ
πΈ-constrained MCF10A model, most of the ππ,πΆππ
πΈ-constrained models of the 98
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NCI-60 panel cell lines were also either infeasible, or do not contain the experimentally measured 99
growth rate within the simulated solution space (Fig 3A). 100
As a sensitivity analysis, we included a flexibilization factor ranging from 0-20% for all ππ used as model 101
constraints, and found that t hat this did not play a role in determining model feasibility or the 102
physiological relevance of the simulations (Fig 3A-B). The ππ,πΆππ
πΈ-constrained MCF10A model only 103
produced physiologically relevant simulations when the flexibilization factor was increased to 700%; 104
even at this point, the ππ,πΆππ
πΈ-constrained model of the SR cell line still performed poorly (Fig 3C). 105
Organization of the feasible flux space 106
We then took the ππ,π
πΈπΊπ-constrained MCF10A model as described above, and added a constraint of 107
the biomass production reaction with the experimentally measured growth rate , to produce a 108
constrained GEM of the MCF10A cell line that makes use of all available data. We used this model to 109
explore the feasible flux space of the entire metabolic network of the cell . Following FVA for every 110
metabolic reaction, we calculated the fractional representation of different metabolic subsystems in a 111
sliding window of 200 reactions, ordered by increasing flux variability (Fig 4; Supplemental Table 3). 112
This analysis showed that metabolic subsystems related to fatty acid metabolism , including for 113
example fatty acid biosynthesis pathways and beta oxidation pathways, exhibited low variability in 114
reaction flux (Fig 4). In contrast, amino acid metabolism (AAM) and most central carbon metabolism 115
(CCM) pathways showed intermediate to high levels of variability (Fig 4) , even though the exo -116
metabolite exchange fluxes used as model constraints were all related to CCM (glucose, lactate) and 117
AAM, consistent with previous observations (13,18). For nucleotide metabolism, we observed two 118
distinct regions in this analysis , one with intermediate variability and another with high variability. 119
Finally, we found that reactions in sphingolipid and steroid metabolism, as well as miscellaneous 120
reactions such as pool reactions and artificial reactions necessary for model simulations, exhibited high 121
flux variability (Fig 4). 122
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Discussion
123
Understanding human cell metabolism at the systems level is of critical interest in many areas of health 124
and medicine. GEM-based simulations have shown very promising applications in microorganisms (9β125
11), but obtaining the necessary input data in human cells has proven to be difficult. A number of 126
methodologies have been developed to leverage transcriptomics data as model constraints (19β23), 127
with mixed results (24), likely because metabolic fluxes are poorly reflected by the abundance of 128
(transcripts of) enzymes in a cell. More recently, exo -metabolite exchange fluxes have been used 129
(3,9,13,25), based on a comparison of exo-metabolite concentrations between the βspentβ and βfreshβ 130
media (4,13). The caveat of this method is that it violates the steady-state assumption of FBA and FVA, 131
and thus should be used with caution. To address this limitation, here we determined exo-metabolite 132
exchange fluxes by collecting multiple samples exclusively during exponential growth phase (Fig 1B-C). 133
Our results indicated a substantial difference in exchange fluxes in different phases of cell growth (Fig 134
2), underscoring the importance of distinguishing between growth phases when studying cell 135
metabolism. With the exponential growth -phase exchange fluxes as model constraints, GEM 136
simulations were biologically meaningful, with the measured cell growth rate falling within the 137
simulated solution space (Fig 3). This allowed us to explore the entire metabolic network of the cell 138
with a physiologically relevant flux profile, revealing a distinct organization of the feasible flux space 139
by metabolic subsystems (Fig 4). 140
Previously, cell-specific GEMs constrained by the exchange fluxes of glucose, lactate, and threonine (all 141
calculated by the CORE method), were shown to predict the cell growth rate to a reasonable degree 142
of agreement with experimentally measured cell growth rates (3). However, incorporation of 143
additional (CORE-calculated) exo-metabolite exchange fluxes, with a flexibilization factor of up to 20%, 144
lead to a large number of infeasible models (Fig 2A-B); suggesting underlying problems with the model 145
constraints and the biological relevance of the simulations. With the REGP method, model simulations 146
remained feasible with a larger number of measured exo-metabolite exchange fluxes, and the feasible 147
flux space was constrained to a biologically meaningful region (Fig 2). We found that the maximum in 148
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silico growth rate exceeded the experimentally determined growth rate by approximately 2-fold (Fig 149
3A-B). This suggests that a portion of the consumed nutrients is diverted into non-growth related 150
metabolic tasks, consistent with the notion that, perhaps with the exception of fast -growth cancer 151
cells, human cells do not operate to solely maximize growth (24,26). 152
Our results show that, even though the input constraints of our model were all related to central 153
carbon metabolism (glucose, lactate) or amino acid metabolism (see Fig 1C), there is nevertheless an 154
intermediate level of flux variability in these subsystems (Fig 4). This is in line with previous work 155
showing that these subsystems do not operate at full capacity in growing cells (18,27). In contrast, we 156
found that reactions in fatty acid metabolism exhibit ed low flux variability, while reactions in 157
sphingolipid metabolism and steroid metabolism exhibited high flux variability, likely reflecting the 158
degrees of connectivity (i.e. pathway branching) in these subsystems (3,28). 159
Our findings demonstrate that constraining GEMs with exo-metabolite exchange fluxes calculated by 160
the REGP method allows for accurate model simulations . While this approach demands more 161
resources for exo-metabolite measurements, we believe that it is crucial to profile the metabolic fluxes 162
of human cells at the genome-scale, which can lead to a better understanding of the metabolic process 163
in healthy cells and the identification of potential metabolic targets in diseases. 164
165
Methods
166
Cell culture 167
MCF10A cells were purchased from ATCC (Cat# CRL-10317). Cells were cultured in DMEM/F12 (Cat# 168
11320033, Gibco) supplemented with MEGM Mammary Epithelial Cell Growth Medium SingleQuots 169
Kit (Cat# CC-4136, Lonza) without GA-1000, along with 0.1 Β΅g/mL cholera toxin (Cat# BML-G117, Enzo 170
Life Sciences) and 100 U/mL penicillin -streptomycin (Cat# 15140, Gibco). Cells were tested for 171
mycoplasma contamination routinely. 172
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Cell proliferation assays 173
Absolute cell counts were measured at 22, 26, 30, 46, 50, and 54 h after seeding using the CyQUANT 174
Cell Proliferation Assay kit (Cat# C7026, ThermoFisher Scientific) with a CLARIOstar Plus plate reader 175
(BMG LABTECH). Cell proliferation at all other time points were measured by Incucyte ZOOM (Essen 176
Bioscience), then converted to absolute cell counts based on the corresponding cell counts from the 177
CyQUANT measurements. 178
Biomass determination 179
Cells were harvested with 0.05% trypsin-EDTA (Cat# 25300054, Gibco) and counted using 0.4% trypan 180
blue (Cat# 15250061, Gibco) in a TC20 Automated Cell Counter (BioRad). The cell suspension was 181
transferred into pre -weighed Eppendorf tubes and pelleted by centrifugation at 200 g for 5 mins. 182
Pellets were dried in a microwave at 360 W for 20 mins, and desiccated in a desiccator for >3 days. 183
Exo-metabolite measurements 184
Sampling for exo-metabolites was done during cellular exponential growth phase between 22 -30 h 185
after seeding by collection of culture supernatant. Glucose and lactate concentrations were quantified 186
as described before (29), using an HPLC (Shimadzu) with an Aminex HPX-87H column (Cat# 1250140, 187
BioRad) at 65 Β°C and an IR detector. The column was eluted with 5 mM H2SO4 at a flow rate of 0.6 188
mL/min for 26 min. Amino acids were quantified as described before (30), with the aTRAQ Kit (Cat# 189
4442673, AB Sciex) using a Nexera UHPLC system (Shimadzu) coupled to a Qtrap 6500+ system (AB 190
Sciex) with a BEH C18 column (150 x 2.1 mm, 1.7 οm) (Cat# 186002353, Waters) at 50 Β°C. A gradient 191
elution of water (eluent A) and methanol ( eluent B), both containing 0.1% formic acid and 0.01 % 192
heptafluorobutyric acid, were used as the mobile phases with a constant flow of 1 mL/min . The 193
following MS parameters were used: Curtain Gas: 50; Collision Gas: Medium; IonSpray Voltage: 5500 194
V; Temperature: 500 Β°C; Ion Source Gas 1: 60; Ion Source Gas 2: 50. The gradient method was: 2% B 195
from 0β2.5 min, 2% to 40% B from 2.5β3.9 min, held at 40% B until 4.2 min, 40% to 90% B from 4.2β196
6.0 min, held at 90% B until 6.1 min, 90% to 2% B from 6.1β8.0 min. Data acquisition and processing 197
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were performed using Analyst and MultiQuant 3.0.3 software. Following data QC, exo -metabolite 198
exchange fluxes (ππ) were calculated by CORE (4) or REGP (see below). 199
Exo-metabolite exchange flux (ππ) calculation by REGP 200
Exo-metabolite exchange fluxes (ππ) were determined by calculating the ratio between spent media 201
and unused media samples, then normalizing to the known metabolite concentrations of the cell 202
culture media (DMEM/F12). Exo-metabolite concentrations were normalized for culture volume and 203
cell dry weight , and a linear model was fitted to regress the concentrations against time. ππ,π
πΈπΊπ is 204
then taken as the slope of the linear model, i.e. the derivative of the fitted metabolite concentration 205
[πΜ] with respect to time π‘ (Fig 1B). Goodness of fit was determined by R 2, with an arbitrary cutoff of 206
0.7. 207
RNA sequencing 208
RNA was sampled at 27 h after seeding. RNA was extracted using the Quick-RNA Microprep Kit (Cat# 209
R1051, Zymo Research) according to the manufacturerβs protocol. Libraries were prepared from 300 210
ng RNA with the KAPA RNA HyperPrep Kit with RiboErase (HMR) (Cat# KK8502, Kapa Biosystems). RNA 211
fragmentation was performed for a desired library insert size of 200-300 bp by fragmentation for 6 min 212
at 94 Β°C. Library concentrations were determined using the Qubit HS kit (Cat# Q32854, Invitrogen). 213
Library size distribution was determined using a High Sensititivy DNA analysis (Cat# 5067-4626, 214
Agilent) on a Bioanalyzer 2100 (Agilent). Libraries with an average between 300 -400 bp were loaded 215
on the NextSeq 2000 system (Illumina). Reads were quality controlled, mapped to the human genome 216
hg38, and counted by Seq2science (31), available at https://github.com/vanheeringen-217
lab/seq2science. 218
Genome-scale metabolic modeling 219
The consensus Human-GEM, Human1 v1.12.0 (3), was used for all procedures detailed below. Human-220
GEM is a βgenericβ model which contains all observed metabolites and reactions in human cells. For 221
each cell line, contextualized models were constructed using tINIT (16), where the generic Human -222
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GEM is pruned in a cell line-specific manner based on whether or not the (transcript of) an enzyme is 223
expressed. We used transcriptomics data measured in-house (MCF10As) or mined from CCLE (17), with 224
an arbitrary expression level cutoff of 1 TPM . Each cell line-specific model was first constrained with 225
components of the growth media (without specifying the exchange fluxes), and then constrained by 226
the measured exchange fluxes with a flexibilization factor ranging from 0% to 700%. For simulation of 227
growth rate, the range of feasible in silico growth rate was simulated by sequentially minimizing and 228
maximizing the biomass reaction, as implemented in the COBRA toolbox (32). The MCF10A-specific 229
model was further constrained with the measured growth rate to perform FVA for all reactions. The 230
flux variability for each reaction, i.e. max(flux) β min(flux), is sorted from lowest to highest. A sliding 231
window of 200 reactions with a step size of 10 reactions was used to assess the variation in reaction 232
flux across different subsystems. Z-scores were calculated for the fraction of reactions per subsystem 233
in a given window. Exchange reactions, transport reactions, and subsystems with less than 5 reactions, 234
were excluded from the visualization of this analysis in Fig 4. All simulations were performed using 235
MATLAB 2023a (MathWorks, Inc.) with Gurobi solver v10.0.1 (Gurobi Optimizer). 236
Data and code availability 237
Raw RNAseq data are available a t GEO, accession GSE293588. All other data and code used in this 238
paper are available in the GitHub repository (https://github.com/Radboud-YuLab/FluxProfilingREGP). 239
Procedures related to metabolic modeling are implemented in MATLAB (2023a). Numerical analyses 240
and graphics are done in R v4.2.3. 241
Acknowledgements
242
The Yu lab is supported by grants from the Dutch Cancer Society and the Radboud -Western 243
Collaboration Fund. We thank Niky Thijssen for technical support during the experimental work. 244
Author contributions 245
Conceptualization: RY . Data curation: CH, XJ. Formal analysis: CH, XJ. Funding acquisition: YC, RY . 246
Supervision: YC, RY . Writing β original draft: CH. Writing β review and editing: XJ, YC, RY . 247
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Competing interests 248
None. 249
250
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Figures and figure legends 251
252
Figure 1. Exo-metabolite exchange fluxes. (A-B), schematic overview of exo-metabolite exchange flux 253
calculation by the CORE and REGP methods. [π], exo-metabolite concentration; A, area under the 254
curve; [πΜ], linear-regression-fitted exo-metabolite concentration (see Methods section) . (C), exo-255
metabolite exchange fluxes (ππ) for 11 cell lines in the NCI-60 panel calculated by the CORE method, 256
and for the MCF10A cell line calculated by either the CORE or the REGP method. 257
258
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259
Figure 2. Exo-metabolite exchange fluxes in different growth phases. (A), growth curve of MCF10A cells 260
showing a distinct lag phase (blue box) and an exponential growth phase (red box and red line). (B-C), 261
ππΊππ’ and ππΊππ¦ showing distinct metabolic profiles during the lag phase and the exponential growth 262
phase. The REGP method is used to calculate the exchange fluxes during the exponential phase (solid 263
red line). Exchange fluxes in the lag phase is estimated by connecting a straight line from the fresh 264
media sample at t=0 h, to the projected exo -metabolite concentration at t=15 h based on REGP 265
calculations (blue dashed line). 266
267
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268
Figure 3. FVA simulation of cell growth rates. (A-C), each cell line-specific GEM model was constrained 269
with the corresponding cell line -specific exo-metabolite exchange fluxes ( ππ) with a flexibilization 270
factor of 0% (A), 20% (B), and 700% (C). Black bars, FVA-simulated minimum and maximum in silico 271
cell growth rate for each cell line. Red dots, experimentally measured growth rate for each cell line. 272
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273
Figure 4 . Organization of the feasible flux space of MCF10A cells. The MCF10A -specific GEM was 274
constrained with ππ,π
πΈπΊπ and the measured growth rate, both with a flexibilization factor of 20%. FVA 275
was performed to determine the flux variability (i.e. the feasible solution space) for every metabolic 276
reaction. The fraction of each metabolic subsystem was calculated in a sliding window of 200 reactions 277
of increasing flux variability, followed by a z-score transformation to facilitate comparison. For ease of 278
visualization, z-scores of > 3 or < -3 were set to 3 or -3, respectively. 279
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