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LETTER doE10.1038/nature14971
A spatial model predicts that dispersal and cell
turnover limit intratumour heterogeneity
Bartlomiej WaclawI, Ivana Bozic13, Meredith E. Pittman'', Ralph H. Hruban4, Bert Vogelstein“ & Martin A. NowaIc2-1.6
Most cancers in humans are large, measuring centimetres in We first model the expansion of a metastatic lesion derived from a
diameter, and composed of many billions of cells'. An equivalent cancer cell that has escaped its primary site (for example, breast or
mass of normal cells would be highly heterogeneous as a result of colorectal epithelium) and travelled through the circulation until it
the mutations that occur during each cell division. What is remark- lodged at a distant site (for example, lung or liver). The cell initiating
able about cancers is that virtually every neoplastic cell within a the metastatic lesion is assumed to have all the driver gene mutations
large tumour often contains the same core set of genetic altera- needed to expand. Motivated by histopathological images (Fig. la), we
tions, with heterogeneity confined to mutations that emerge late model the lesion as a conglomerate of balls of cells (see Methods and
during tumour growth'''. How such alterations expand within the Extended Data Fig. 1). Cells occupy sites in a regular three-dimen-
spatially constrained three-dimensional architecture of a tumour, sional lattice (Extended Data Fig. 2a, b). Cells replicate stochastically
and come to dominate a large, pre-existing lesion, has been with rates proportional to the number of surrounding empty sites
unclear. Here we describe a model for tumour evolution that shows
how short-range dispersal and cell turnover can account for rapid
cell mixing inside the tumour. We show that even a small selective
advantage of a single cell within a large tumour allows the
descendants of that cell to replace the precursor mass in a clinically
relevant time frame. We also demonstrate that the same median-
isms can be responsible for the rapid onset of resistance to chemo-
therapy. Our model not only provides insights into spatial and
temporal aspects of tumour growth, but also suggests that target-
ing short-range cellular migratory activity could have marked
effects on tumour growth rates.
Tumour growth is initiated when a single cell acquires genetic or
epigenetic alterations that change the net growth rate of the cell (birth
minus death), and enable its progeny to outgrow surrounding cells. As
these small lesions grow, the cells acquire additional alterations that
cause them to multiply even faster and to change their metabolism to
survive better the harsh conditions and nutrient deprivation. This
progression eventually leads to a malignant tumour that can invade d
surrounding tissues and spread to other organs. Typical solid tumours
contain about 30-70 clonal amino-acid-changing mutations that have
accumulated during this multi-stage progression'. Most of these muta-
tions are believed to be passengers that do not affect growth, and only
—5-10% are drivers that provide cells with a small selective growth
advantage. Nevertheless, a major fraction of the mutations, particu-
larly the drivers, are present in 30-100% of neoplastic cells in the
primary tumour, as well as in metastatic lesions derived from it's.
Figure I I Structure of solid neoplasms. a, Hepatocellular carcinoma
Most attempts at explaining the genetic make-up of tumours composed of balls of cells (circled in green) separated by non-neoplastic tissue
assume well-mixed populations of cells and do not incorporate spatial (asterisk). b, Adjacent section of the bottom tumour in a immunolabelled
constraintr'°. Several models of the genetic evolution of expanding with the proliferation marker Ki67. The edge ofthe tumour is delineated in red;
tumours have been developed in the past"-' 4, but they assume either the centre is marked with a green circle. Proliferation is decreased in the centre
very few mutations' or one- or two-dimensional growth".". when compared to the edge of the neoplasm. c, d, Higher magnification of
Conversely, models that incorporate spatial limitations have been the centre (c) and the edge (d) with each proliferating neoplastic cell marked
developed to help to understand processes such as tumour metabolism1s, by a green dot. The blue nuclei without green dots are non-proliferating. The
angiogenesism" and cell migration", but these models ignore gen- red circle in c demonstrates an example of cells (inflammatory cells) that
were not included in the count of neoplastic cells. The neoplastic tissue in
etics. Here, we formulate a model that combines spatial growth and d is above the red line; non-neoplastic (normal liver) is below the red
genetic evolution, and use the model to describe the growth of primary line. Comparison of c with d shows that proliferation of neoplastic cells is
tumours and metastases, as well as the development of resistance to decreased in the centre as compared to the edge of the lesion (quantified in
therapeutic agents. Extended Data Table I).
'School of Physics end Astronomy. Univesity of Edinburgh Olt Peter Guthrie Tad Reed. Echnburei CH9 ND. UK.2Prowaen for Evolutonery Dynamics, Harvwd University. One Battle Square.
Cambridge. Massachusetts 02138. USA. aDepartment et Mathematics. lianrard thwersity. One Oxford Street. Cambridee. Massachusetts 02133. USA' he Sol Goldman Pancreatic Cancer Research
Center. Department et Palk...sly. Johns Flocains University Sdicee of Medicine. 401 North Broadway. Weinberg 2202. Baltimore. Maryland 21231.USA SLucleig Center and Howard Hushes medial
InSlittite, Johns Hopkins Kimmel Cancer Center. 1650 Oriws Street Bellmore. Maryland 21287. USA. `Department oe Organismicand Evolubonary Ulm/. Renard Unmake. 26 Word Street
Cambridge. Massashusetts 02138. USA.
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RESEARCH LETTER
(non- neoplastic cells or extracellular matrix), hence replication is Non-spatial models point to the size of a tumour as a crucial deter-
faster at the edge of the tumour. This is supported by experimental minant of chemotherapeutic drug resistance'''. To determine
data (Fig. I b-d and Extended Data Table I). A cell with no cancer cell whether a spatial model would similarly predict this dependency in
neighbours replicates at the maximal rate of b = In(2) = 0.69 days-I, a clinically relevant time frame, we calculated tumour regrowth prob-
in which b denotes the initial birth rate, equivalent to 24h cell- abilities after targeted therapies. We assume that the cell that initiates
doubling time, and a cell that is completely surrounded by other cancer the lesion is susceptible to treatment, otherwise the treatment would
cells does not replicate. Cells can also mutate, but we assume all muta- have no effect on the mass, and that the probability of a resistant
tions are passengers (they do not confer fitness advantages). After mutation is 10- ' (Methods); only one such mutation is needed for a
replication, a cell moves with a small probability (M) to a nearby place regrowth.
close to the surface of the lesion and creates a new lesion. This 'sprout- Figure 3a shows snapshots from a simulation (Supplementary
ing of initial lesions could be due to short-range migration after an Video I) performed before and after the administration of a typical
epithelial-to-mesenchymal transition" and consecutive reversion to a targeted therapy at time T= 0. At first, the size of the lesion (-3 mm at
non-motile phenotype. Alternatively, it could be the result of another T= 0) rapidly decreases, but I month later resistant clones begin to
process such as angiogenesis (Methods), through which the tumour proliferate and form tumours of microscopic size. Such resistant sub-
gains better access to nutrients. The same model governs the evolution clones are predicted to be nearly always present in lesions of sizes that
of larger metastatic lesions that have already developed extensive vas- can be visualized by clinical imaging techniquesS12. By 6 months after
culature. Cells die with a death rate (d) independent of the number of treatment, the lesions have regrown to their original size. The evolu-
neighbours, and are replaced by empty sites (non-neoplastic cells tion of resistance is a stochastic process—some lesions shrink to zero
within the local tumour environment). and some regrow (Extended Data Fig. 4a). Figure 3b, c shows the
If there is little dispersal (M .6 0), the shape of the tumour becomes probability of regrowth versus the time from the initiation of the lesion
roughly spherical as it grows to a large size (Fig. 2a and Supplementary to the onset of treatment upon varying net growth rates b-d and
Video 2). However, even a very small amount of dispersal markedly dispersal probabilities. Regardless of growth rate, the capacity to
affects the predicted shape. For M> 0, the tumour forms a conglom- migrate makes it more likely that regrowth will occur sooner, particu-
erate of `balls' (Fig. 2b, Extented Data Fig. 2c and Supplementary larly for more aggressive cancers, that is, those which have higher net
Video 3), much like those observed in actual metastatic lesions, with growth rates (Fig. 3b). This conclusion is in line with recent theoretical
the balls separated by islands of non- neoplastic stromal cells mixed work on evolving populations of migrating cells''. If resistant muta-
with extracellular matrix. In addition to this remarkable change in tions additionally increase the dispersal probability before or during
topology, dispersal strongly affects the growth rate and doubling time treatment, regrowth is faster (Extended Data Fig. 4b, c).
of the tumour. Although the size (N) of the tumour increases with time Having shown that the predictions of the spatial model are consist-
(7) from initiation as without dispersal (Extended Data Fig. 3a, b), ent with metastatic lesion growth and regrowth times, we turn to
it grows much faster (—exp(const X 7) for large 7) when M> primary tumours. In contrast to metastatic lesions, here the situation
(Fig. 2c). This also remains true for long-range dispersal in which M is considerably more complex because the tumour cells are continually
affects the probability of escape from the primary tumour into the acquiring new driver gene mutations that can endow them with fitness
circulation to create new lesions in distant organs (metastasis). advantages over adjacent cells within the same tumour. Our model of a
Using plausible estimates for the rates of cell birth, death and dispersal primary tumour assumes that it is initiated via a single driver gene
probability, we calculate that it takes 8 years for a lesion to grow from mutation that provides a selective growth advantage over normal
one cell to one billion cells in the absence of dispersal (Al = 0), but less neighbouring cells. Each subsequent driver gene mutation reduces
than 2 years with dispersal (Fig. 2c). The latter estimate is consistent the death rate as d = b(l — s)k, in which k is the number of driver
with experimentally determined rates of metastasis growth as well mutations in the cell (k a 0, and s is the average fitness advantage
as clinical experience, while the conventional model (without dis- per driver. Almost identical results are obtained if driver gene muta-
persal) is not. tions increase cell birth rather than decrease cell death, or affect both
a Figure 21 Short-range dispersal affects size,
shape and growth rate of tumours. a. b. A
spherical lesion in the absence of dispersal (M = 0)
(a) and a conglomerate oflesions (b), each initiated
by a cell that has migrated from a previous
lesion, for low but non-zero migration(M = 10-6).
Colours reflect the degree of genetic similarity
cells with similar colours have similar genetic
alterations. The death rate is d = 0.8b,
which corresponds to a net growth rate of
0.26 = 0.14 days- I, and N = 10' cells. c, Dispersal
(M > 0) causes the tumour to grow faster in
time. Each point = 100 sanples, error bars (too
small to be visible) areIn. Continuous lines
(extrapolation) arc 6,000 X 100.43T (gee,)
1,000 X 100 77. (blue).
1010
M=10-5
102
0 10 20 30 40 50 60
T (months)
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LETTER RESEARCH
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Figure 4 Genetic diversity is strongly reduced by the emergence of driver
T (month) T(month)
mutations. a-f. For all, M = 0 and the initial net growth rate = 0.007 clays-1
Figure 3 I Treatment success rates depend on the net growth rate of (d = 0.996). The three most abundant genetic alterations (GAs) have been
tumours. a, Time snapshots before and during therapy (M = Resistant colour-coded using red (R), green (G) and blue (8) (c). Each section is 80 cells
subpopulations that cause the tumour to regrow after treatment can be seen thick. Combinations of the three basic colours correspond to cells having two or
at T = I month. b, c, Probability of tumour regrowth (P,g,„,$) as a function three of these genetic alterations. a, No drivers—separated, conical sectors
of time after treatment initiation, for different dispersal probabilities (M) and emerge in different parts of the lesion, each corresponding to a different clone.
net growth rates of the resistant cells. A higher net growth rate (b) leads to b, Drivers with selective advantage s = 1% lead to clonal expansions and
a high regrowth probability, so that 50% of tumours regrow 6 months after many cells have all three genetic alterations (white area). d Genetic diversity
treatment is initiated when M = I 0-5. c., Tumours with lower net growth rates can be determined quantitatively by randomly sampling pairs ofcells separated
require >20 months to achieve the same probability of regrowth. Number of by distance r and counting the number of shared genetic alterations. e, The
samples = Ito 800 per point (282 on average). Error bars areM. Sec number of shared genetic alterations versus the normalized distance il<r>
Methods for details. decreases much more slowly for the case with (red) than without (blue) driver
mutations. f, The total number of genetic alterations present in at least
50% of all cells is much larger for s = 1% than for s = 0%. Number of
cell birth and cell death (Extended Data Fig. 514; the most important samples = 50 per data point. Error bars arc M.
parameter is the fitness gain, s, conferred by each driver mutation.
Figure 4a shows that in the absence of any new driver mutations (as historically been viewed as a feature of cancer associated with late
for a perfectly normal cell growing in utero), donal subpopulations events in tumorigenesis, such as invasion through basement mem-
would be restricted to small, localized areas. Each of these areas has at branes or vascular walls, this classical view of migration pertains to
least one new genetic alteration, but none of them confers a fitness the ability of cancer cells to migrate over large distance?'. Instead, our
advantage (they are 'passengers'). In an early tumour, in which the analysis reveals that even small amounts of localized cellular move-
centre cell contains the initiating driver gene mutation, the same struc- ment are able to markedly reshape a tumour. Moreover, we predict
ture would be observed—as long as no new driver gene mutations have that the rate of tumour growth can be substantially altered by a change
yet appeared. The occurrence of a new driver gene mutation, however, in dispersal rate of the cancer cells, even in the absence of any changes
markedly alters the spatial distribution of cells. In particular, the het- in doubling times or net growth rates of the cells within the tumour.
erogeneity observed in normal cells (Fig. 4a) is substantially reduced Some of our predictions could be experimentally tested using new cell
(Fig. 4b and Supplementary Video 5). The degree of heterogeneity can labelling techniques'''. Our results could also greatly inform the
be quantified by calculating the number of genetic alterations (passen- interpretation of mutations in genes whose main functions seem to
gers plus drivers) shared between two cells separated by various dis- be related to the cytoskeleton or to cell adhesion rather than to cell
tances (Fig. 4d-f). The genetic diversity is markedly decreased (Fig. 4e), birth, death, or differentiationn". For example, cells that have lost the
even with relatively small fitness advantages (s = 1%). This also has expression of E-cadherin (a cell adhesion protein) are more migratory
implications for the number of genetic alterations that will be present than normal cells with intact E-cadherin expression", and loss of
in a macroscopic fraction (for example, >50%) of all cells. Figure 4f E-cadherin in pancreatic cancer has been associated with poorer pro-
shows that this number is many times larger for s = I% than s = 0%. gnosis", in line with our predictions.
Furthermore, our model predicts that virtually all cells within a large
Online Content Methods along with any additional Extended Data display items
tumour will have at least one new driver gene mutation after 5 years of and Source Data. are available in the online version of the paper: references unique
growth (Extended Data Fig. 5a).The faster the clonal expansion occurs to these sections appear only in the online paper.
(the larger s is), the smaller the number of passenger mutations
(Extended Data Fig. 5d, e). Our results are also robust to changes to Received 1September 2014: accepted 23 July 2015.
the model (Methods and Extended Data Figs 5 and 6). We stress that Published online 26 August 2015.
an important prerequisite for limiting heterogeneity is cell turnover in 1. Vogelstein.B. eta?. Cancergenome landscapes. Science 339,1546-1558(2013).
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can 'percolate through the tumour only if they replace other cells. In pancreatic cancer. Nature 467,1114-1117 (2010)
the absence of cell turnover, tumours are much more heterogeneous 3. Sottoriva.A.et at Intiatumor heterogeneity in human glicblastoma reflects cancer
evolutionanidynamia, Proc. NatI Acad. Sci USA 110.4009-4014 (2013)
(Extended Data Fig. 6d). 4. Navin. N. eta?. Tumour evolution inferred by single-cell sequencing. NaMe 472,
In summary, our model accounts for many facts observed clinically 90-94 (2011)
and experimentally. Our results are robust and many assumptions can 5. Gerlinger. M. et at Intratumor heterogeneity and branched evolution revealed by
multiregion sequencing. N. Engl.I Med 366,883-892 (2012).
be relaxed without qualitatively affecting the outcome (Methods and & Gatenby.R.A & Vincent.T.L.An evolutionary modelof carcinogenesis.CancerRes
Supplementary Information). Although tumour cell migration has 63.6212-6220 (2003).
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RESEARCH LETTER
7. Johnston. M. D.. Edwards. C. M. Balmer. W. F. Maini. P. K. & Chapman, S.J.
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28 Lawson. C. D. & Burridge. K The on-off relationship of Rho and Rac during
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15. Kim.Y..Magdalena.A.S&Othrner.H.G.A hybridmodelkr tumor.spheroid growth Supplementary Information is available in the online version of the paper.
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17.1773-1798(2007). Acknowledgements Support from The John Templeton Foundation is gratefully
16. McDougall. S R., Anderson, A. R. & Chaplain. M.A Mathematical modeling of acknowledged B.W. was supported by the Leverhulme Trust Eery-Career Fellowship.
dynamic adaptive tumour-induced angicgenesis: clinical implications and and the Royal Society of Edinburgh Personal Research Fellowship. 1.8. was supported
therapeutic targeting strategies. J. Meer. Blosi. 241, 564-589 (2006). by FoundationalQuestions in Evolutionary Bio Grant
17. Hawkins-Deemer, A.. Rockne. R. C..Anderson, A. RA & Swanson. K FL Modeting S.M.acknowledge support from The Virginia and M. Ludwig Fund for Cancer
tumor-associated edema in gliomas during anti-angiogenic therapy and its Research. The Lustgarten Foundation for Pancreatic Cancer Research. The Sd
imnact nn imao4:444tornnr Pm& Chun( 2 SA ontm, Goldman Center for Pancreatic Cancer Research. and Nil grants CA43460 and
CA62924.
Author Contributions I.B. and B.Y. designed the study. B.W.wrote the
computer pr ams and made simulations. B.W.. I.B. andfl made analytic
calculations.= and R.H.H.canied out experimental work All authorsdiscussed the
results. The man uscr_S_was written primarily by B.W.,=. I.B. and BV.. with
ISOZIC. Liven. U.& NOWalt.IA A LlytlatOKS Ot targeted cancer tnerapy. MOOS I1101. contributions from= and R.H.H.
Med.18. 311-316 (2012).
21. Bozk, L& Nowak M. A.Timirg and heterogeneity of mutations associated with Author Information Re .nts and perrnissions information is available at
drug resistance in metastatic cancers.Proc. NatfAcad. Sci. USA 111. The authors declare no competing financial interests.
15964-15968 (2014). Readers are welcome to comment on the online version of the paper.
22 Turke, A. B. et aL Preexistence and clonal selection of MET amplification in EGFR Cares ndence and requests for materials should be addressed to=
mutant NSCLC. Cancer CO 17, 77-88 (2010).
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LETTER
METHODS bacterial colonies"' show that the structure of the lattice (or the lack thereof in
No statistical methods were used to predetermine sample size. Experiments were off-lattice models) has a marginal effect on genetic heterogeneity.
not randomized and investigators were not blinded to allocation during experi- Asynchronous cell division. Division times ofrelated cells remain correlated for a
ments and outcome assessment few generations. However, stochastic cell division implemented in our model is a
Spatial model for tumour evolution. Tumour modelling has a long tradition". good approximation for a large mass of cells and is much less computationally
Many models of spatially expanding tumours were proposed in the past"'"', expensive than modelling a full cell cycle.
but they either assume very fewn-m-s'-"."."-" or no new mutations at allumat".". Replication faster at the boundary than in the Interior. Several studies have
or one- or two-dimensional growthwwn'". On the other hand, well-mixed described a higher proliferation rate at the leading edge of tumours, and this has
models with several mutations'" do not often include space, and computa- been associated with a more aggressive clinical course". To estimate the range of
tional models aimed at being more biologically realistic"' require too much values of death rate d for our model. we used the proliferation marker Ki67.
computing resources (time and memory) to simulate realistically large tumours Representative formalin-fixed, paraffin-embedded tissue blocks were selected
(N., 10' cells). Our model builds on theEden latticemodel' and combines spatial from four small chromophobe renal cell carcinomas and six small hepatocellular
growth and accumulation ofmultiple mutations. Since we focus on the interplay of carcinomas by the pathologist (=.). A section of each block was immunola-
genetics. spatial expansion and short-range dispersal of cells. for simplicity we do belled for IC67 using the Ventana Benchmark XT system. Around 8-12 images.
not explicitly model metabolism". tissue mechanics, spatial heterogeneity of tis- depending on the size of the lesion, were acquired from each tumour. Fields were
sues, different types of cells present or angiogenesis". chosen at random from the leading edge and the middle of the tumour and were
A tumour is made ofnon-overlapping balls (microlesions) ofcells. Tumour cells not necessarily 'hot spots' of proliferative activity. Using an Image) macro, each
occupy sites of a regular 3D square lattice(Moore neighbourhood, 26 neighbours). Ki67-positive tumour nucleus was labelled green by the pathologist. and each
Empty lattice sites are assumed to be either normal cells or filled with extracellular Ki67-negative tumour nucleus was labelled red. Other cell types (endothelium,
matrix and are not modelled explicitly. Each cell in the model is described by its fibroblasts and inflammatory cells) were not labelled. The proliferation rate was
position and a list of genetic alterations that have occurred since the initial neo- then calculated using previously descrthed methods". Statistical significance ofthe
plastic cell, and the information about whether a given mutation is a passenger. results was determined using a Kolmogorov-Smimov nap-sample test (signifi-
driver. or resistance-carrying mutation. A passenger mutation does not affect the cance level 0.05). The study was approved by the Institutional Review Board of the
net growth rate whereas a driver mutation increases it by disrupting tight regu- Johns Hopkins University School of Medicine. In all ten tumours, the proliferation
lation ofcellular divisions and shifts the balance towards increased proliferation or rate at the leading edge of the tumour was grmter than that at the centre by a factor
decreased apoptosis. The changes can also be epigenetic and we do not distinguish of 1.25 to 6 (Extended Data Table I). Comparing the density of proliferating cells
between different types of alterations. We assume that each genetic alteration to our model gives cf.., 0.56 (range: d = 0.176...0.86), which is what we assume in
occurs only once ('infinite allele model"). The average numbers of all genetic the simulations of aggressive lesions.
alterations, driver and resistant genetic alterations produced in a single replication Equal fitness of all cells in metastatic lesions. We assume that cells in a meta-
event are denoted by y, 7d. and yr. respectively. When a cell replicates, each of the static lesion are already very fit since they contain multiple driven. Indeed. studies
daughter cells receives n new genetic alterations of each type (n being generally ofprimary tumours and their matched metastases usually fail to find driver muta-
different in both cells)drawn at random from the Poisson probabilitydistribution: tions present in the metastases that were not present in the primary lesions'',
although there are notable exceptions, see, for example. refs 75 and 76.
e-712(11.12)" Experimental evidence in microbes" and (to a lesser extent) in eukaryotes" sug-
POO — (I)
n! gests that fitness gains due to individual mutations are largest at the beginning of
in which x denotes the type of genetic alteration. an evolutionary process and that the effects oflater mutations are much smaller.It
In model A shown in Figs 2-1. replication occurs stochastically. with rate remains to be seen how well these results apply to late genetic alterations in
proportional to the number of empty sites surrounding the replicating cell. and cancer" but if true. new driven occurring in the lesion are unlikely to spread
death occurs with constant rate depending only on the number of drivers. We also through the population before the lesion reaches a clinically relevant size.
simulated other scenarios (models B, C and D. see below). Driver mutations Dispersant,our model. cells detach from the lesion and attach again at a different
increase the net growth rate (the difference between proliferation and death) either location in the tissue. This can be viewed either as cells migrating from one place to
by increasing the birth rate or decreasing the death rate by a constant factor 1 + s. another one. or as a more generic mechanism that allows tumour cells to get better
in which s> 0. access to nutrients by dispersing within the tissue. hence providing a growth
Dispersal is modelled by moving an offspring cell to a nearby position where it advantage over cells that did not disperse. Some mechanisms that do not involve
starts a new microksion (Extended Data Fig. la). Klicroksions repel each other; a active motion (that is. cells becoming motile) are discussed below.
'shoving algorithm's" (Extended Data Fig. Ib) ensures they do not merge. Migration. Cancer cells are known to undergo epithelial-to-mesenchymal trans-
Code availability. The computer code (available at httpifwww2.ph.ed.ac.uki ition. the origin of which is thought to be epigenetic". This involves a cell becom-
—bwadawfcancer-code) can handle up to 1 X 109 cells. which corresponds to ingmotik and miming some distance. If the cell finds the right environment,it can
tumours that are clinically meaningful and can be observed by conventional switch back to the non-motile phenotype and start a new lesion. Motility can be
medical imaging (diameter >1cm). The algorithm is discussed in details in the enhanced by tissue fluidization due to replication and death". Instead of mod-
Supplementary Information. It is not an exact kinetic Monte Carlo algorithm elling the entire cycle (epithelial-mesenchymal-epithelial). we only model the
because such an algorithm would be too slow to simulate large tumours. A com- final outcome (a cell has moved some distance).
parison with kinetic Monte Carlo for smaller tumours (Supplementary Tumour buds. Many tumours exhibit focally invasive cell clusters, also known as
Information) shows that both algorithms produce consistent results. tumour buds. Their proliferation rate is less than that of cells in the main turnout'.
Model parameters. The initial birth rate 6= In(2) 0.69 days "'. which corre- We propose that tumour buds contain cells that have not yet completed epithdial-
sponds to a 21h minimum doubling time. The initial death rate d = 0...0.995b to.meserichymal transition and therefore they proliferate slower.
depends on the aggressiveness of the tumour (larger values = less aggressive lesion). Single versus cluster migration. Ref. 82 found that circulating cancer cells can
In simulations of targeted therapy. we assume that. before treatment, = 0.69 travel in clusters of 2-50 cells, and that such clusters can initiate metastatic foci.
days"' and d= 0.56 = 0.35 dayss '. whereas during treatment b= 035 days- ' They report that approximately one-halfof the metastatic foci they examined were
and d = 0.69 days- ', that is, birth and death rates swap places This rather arbitrary initiated by single circulating cancer cells, and that circulating cancer cell dusters
choice leads to the regrowth time of about 6 months which agrees well with clinical initiated the other half. The authors also note that the cells forming a duster are
evidence. Mutation probabilities are 7 = 0.02,7d = 1 X 10-5.7, = I X 10-7. in line probably neighbouring cancer cells from the primary tumour. This means that the
with experimental evidence and theoretical work"'". Since there are no reliable genetic make-up of cells within a newly established lesion will be very similar.
data on the dispersal probability M. we have explored a range of values between regardless of its origin (single cell versus a small cluster of cells). Therefore, the
M = 1 X 10-7 and I X 10-1. An parameters are summarized in Extended Data Fig. ability to travel in clusters should not affect the genetic heterogeneity or regrowth
Ic, see also further discussion in Supplementary Information. probability as compared to single-cell dispersal from our modeL
Validity of the assumptions of the modeL Our model is deliberately oversim- Angiogenesis. We do not explicitly model angiogenesis for two reasons. First.
plified. However, many of the assumptions we make can be experimentally jus- most genetic alterations that can either change the growth rate or be detected
tified or shown not to qualitatively affect the model. experimentally must occur at early stages of tumour growth as explained before.
Three-dimensional regular lattice of cells. The 3D Moore neighbourhood was Hence, the genetic make-up of the tumour is determined primarily by what
chosen because it is computationally fast and introduces relatively fever artefacts happens before angiogenesis. Second, local dispersal from the model mimics
related to lattice symmetries. Real tissues are much less regular and the number of tumour cells interspersing with the vascularized tissue and getting better access
nearest neighbours is different". However. recent simulations of similar models of to nutrients, which is one of the outcomes of angiogenesis.
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EFTA00603741
RESEARCH LETTER
Biomechanics of tumours. Growth is affected by the mechanical properties of regression, and some do not. If only resistant cells can migrate, regrowth is faster
cells and the extracellular matrix. We do not explicitly include biomechanics (see, (Extended Data Fig. 4b, c). Extended Data Fig. 4d-g shows regrowth probabilities
however, below).in contrast to more realistic models"". as this would not allow us P,,,,,„„th for different treatment scenarios not mentioned in the main text. depend-
to simulate lesions larger than about 1 X 106 cells. Instead, we take experimentally ing on whether the drug is cytostatic (bite„,tr,„„, = 0) o cytocidal = b).
determined values for birth and death rates. values that are affected by biomecha- and whether d = 0 or d>0 before treatment. In Extended Data Fig. 4d, cells
nics. as the parameters of our model. replicate and die only on the surface. and the core is 'quiescent'—cells are still
Isolated balls of cells. In our simulations. balls of cells are thought to be separated alive there but cannot replicate unless outer layers are removed by treatment
by normal, vascularized tissue which delivers nutrients to the tumour. The envir- (Supplementary Videos 6 and 7). Pitp.0.0 does not depend on the dispersal prob-
onment of each ball is the same. and there are no interactions between the balls ability Af at all. and is close to 100% for N> 108 cells. a size that is larger than for
other than mechanical repulsion. This represents a convenient mathematical con- d > 0 (Extended Data Fig. 40. It can be shown that P,,,,„,„h = 1 — exp(-7,4
trivance and qualitatively recapitulates what is observed in stained sections of Extended Data Fig. 4e is for the cytostatic drug (Oh...um= = 0): this is
actual tumours (Fig. la). We investigated under which circumstances the balls also equivalent to the eytocidal dnigif the tumour has a necrotic core (cells are dead
of cancer cells would mechanically repel each other. see Extended Data Fig. 7 for a but still occupy physical volume). In this case, increases with Af because
graphical summary of the results. We simulated a biomechanical, off-lattice model more resistant cells are on the surface for larger M (cells can replicate only on the
of normal tissue composed of 'ducts' lined with epithelial cells and separated by surface in this scenario). Extended Data Fig. 4f. g shows models with cell death
stroma (Supplementary Information. section 8). Mechanical interactions between present even in the absence of treatment (d = 0.9b) but occurring only at the
cells were modelled using an approach similar to that described previously'". "s surface. unlike in Fig. 3 where cells also die inside the tumour. Death increases
with model parameters taken from refs 59, 60.85-88. We assumed cancer cells to owing to a larger number of cellular division necessary to obtain the same
be of epithelial origin. as are most cancers". Cancer cells that invaded different size and hence more opportunities to mutate.
areas ofepithelium grew into balls that remained separated by thin slices of stroma Relaxing the assumptions of the model. Figure 4 shows that even a small fitness
(Supplementary Videos 8-11). This 'encapsulation' of tumour microlesions was advantage substantially reduces genetic diversity through the process of donal
possible owing to the supportive nature of stroma that is able to mechanically resist expansion, see also Supplementary Videos 4 and S. We now demonstrate that this
expansion of balls of cancer cells. Encapsulation is essential if the balls are to repel also applies to modified versions of the model, proving its robustness.
each other. If the tissue is 'fluidized' by random replication and death. the balk Exact values ofMend s has no qualltathv effect. Extended Data Fig. 8b, e shows
quickly merge (Supplementary Video 12). Another important factor are differ- that the average number of shared genetic
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