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Applied and Environmental Microbiology, September 2000, p. 3868-3877, Vol. 66, No. 9
0099-2240/00/$04.00+0
Copyright © 2000, American Society for Microbiology. All rights reserved.
Mathematical Analysis of Growth and Interaction
Dynamics of Streptomycetes and a Bacteriophage in Soil
N. J.
Burroughs,1,*
P.
Marsh,2 and
E. M. H.
Wellington2
Mathematics Institute1
and Department of Biological Sciences,2
University of Warwick, Coventry CV4 7AL, United Kingdom
Received 24 May 1999/Accepted 24 April 2000
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ABSTRACT |
We observed the infection cycle of the temperate actinophage KC301
in relation to the growth of its host Streptomyces lividans TK24 in sterile soil microcosms. Despite a large increase in phage population following germination of host spores, there was no observable impact on host population numbers as measured by direct plate counts. The only change in the host population following infection was the establishment of a small subpopulation of KC301 lysogens. The interaction of S. lividans and KC301 in soil
was analyzed with a population-dynamic mathematical model to determine the underlying mechanisms of this low susceptibility to phage attack
relative to aquatic environments. This analysis suggests that the soil
environment is a highly significant component of the phage-host
interaction, an idea consistent with earlier observations on the
importance of the environment in determining host growth and
phage-host dynamics. Our results demonstrate that the accepted phage-host interaction and host life cycle, as determined from agar
plate studies and liquid culture, is sufficient for quantitative agreement with observations in soil, using soil-determined rates. There
are four significant effects of the soil environment: (i) newly
germinated spores are more susceptible to phage lysis than are hyphae
of developed mycelia, (ii) substrate mycelia in mature colonies adsorb
about 98% of the total phage protecting susceptible young hyphae from
infection, (iii) the burst size of KC301 is large in soil (>150, 90%
confidence) relative to that observed in liquid culture (120, standard
error of the mean [SEM], 6), and (iv) there is no measurable impact
on the host in terms of reduced growth by the phage. We hypothesize
that spatial heterogeneity is the principal cause of these effects and
is the primary determinant in bacterial escape of phage lysis in soil.
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INTRODUCTION |
The filamentous nature of
streptomycetes causes two problems for their quantification in soil and
interaction with phage. First, the identification of a lysable unit
during phage infection as a proportion of a hypha is unclear; second,
the rate of phage adsorption to hyphae is dependent upon the age of the
hyphae (11, 22, 30). Phage interaction, therefore, changes
over time as a function of colony heterogeneity. The effects of this
heterogeneity are greatest in undisturbed colonies where interactions
are dependent on diffusion. Growth on agar is limited to the boundary
of the colony by the diffusion of nutrients and staling compounds
(33). In contrast, colonies grown in liquid culture have
little spatial heterogeneity since diffusion is rapid, and the uniform
exposure of host to phage can result in efficient phage lysis
(4). The effects of diffusion in soil are expected to be
informed by, but distinct from, both of these cases and possibly
underlies the environmental dependence observed in a number of systems
(15, 17, 28).
Our objective in this study was to use population-dynamic modeling of
the phage-streptomycete interaction to quantify and characterize the
growth of streptomycetes and the efficiency of phage infection in soil.
We examined whether specific growth and interaction characteristics
were attributable to the soil environment.
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THEORY |
The streptomycete life cycle includes germination, colony
formation, and development (vegetative growth), and sporulation (7, 18). In brief, spores germinate via a primary germ tube that undergoes branching after a period of linear extension and nucleoid replication. In Streptomyces coelicolor, mature
colonies grow exponentially (as measured by DNA content) through linear (apical) extension of individual hyphae with an exponential increase in
the number of branches (2). Exponential growth continues until limited through depletion of an essential nutrient, occupancy of
all spatial niches, or the accumulation of staling compounds (3). The nature of growth limitation in soil is unclear.
Sporulation occurs following the formation of aerial mycelia.
Phage can be extracted from the soil environment, with viability
decaying at the rate of 0.1 day
1 (10). Phage
survival therefore requires either continuous production (virulence) or
latency (lysogeny). Phage adsorb to mycelia in a two-step process
(1): a process specific to the phage receptor and a
nonspecific process caused by hydrophobic and electrostatic forces. Specific adsorption may lead to infection and either
lysis or lysogeny. The susceptibility of streptomycetes to phage
infection varies with the age of the mycelia, with older mycelia being
more resistant than young tips (11, 22, 30). This variation
may be due to higher rates of DNA synthesis in hyphal-tip proximal regions (14) or to differences in the density of, or area
covered by, surface receptor molecules (6, 12). The
replication rate of phage therefore depends on the rate of adsorption
to, and infection of, susceptible hosts, transportation processes such
as rates of diffusion of phage, and the burst size of the virus. The
burst size may be affected by the environment (15),
presumably through the nutritional status of the host.
We constructed a model of the lifecycle of the host and phage (Fig.
1) based on mass action adsorption
effects. Colony heterogeneity was modeled by separate compartments for
spores, germlings, and substrate mycelia. A germling is an intermediate
between the spore and the exponentially growing colony and is
physically identifiable as the germ tube and initial branchings (when
growth is linear) prior to the exponential growth in the number of
branches. The relatively slow growth of the germling (compared to the
exponential growth of the colony) means that the germling can be
treated as a nongrowing state. Viable propagules can be lost when
germination fails or when germlings fail to differentiate into viable
substrate mycelia. We defined the probabilities
Pg and Pd for successful germination and differentiation, respectively (Fig. 1). After differentiation, exponential growth of the substrate mycelia commences and ends with saturation of an unknown resource at the "vegetative capacity," denoted by K, intrinsic to the soil and
conditions. K is less than the final soil capacity because
mycelial growth ceases at saturation, while sporulation continues. The
growth rate was modeled with a standard logistic form µ(1
[M/K]), i.e., the growth rate decreases linearly from a
maximum value µ to zero as the total mycelial mass M
approaches the vegetative capacity K. The germlings
and substrate mycelia are divided into susceptible and resistant
compartments, designated Gs,
Gr, Ts, and
Tr, respectively. Germlings and young
tips are initially susceptible and acquire resistance to phage lysis as
they age (Fig. 1).

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FIG. 1.
(A) Schematic representation of the host dynamics.
Germlings and young tips are initially susceptible to phage lysis
(compartments Gs and Ts)
but acquire resistance as they age at rates G
and T, respectively (resistant compartments
Gr and Tr). After
germination, germlings differentiate into exponentially growing
substrate mycelium at rate k. Germlings are viable with
probability Pg and are successful in forming
colonies with probability Pd. If either
probability is <1, then a drop in total propagules occurs after
germination, which can alternatively be described as death rates
g(1 Pg) and k(1 Pd) of spores and germlings, respectively. Germlings
that die still adsorb phage nonspecifically
(Tfail). In the basic model
Pg is 1 and T is large
so that young tips are effectively resistant. (B) Schematic
representation of the phage dynamics interacting with germlings.
Interaction with substrate is similar, with T replacing
G. Phage adsorbs to mycelia in a two-step process:
nonspecific reversible adsorption (forward rate + × mycelium density G, reverse rate  )
producing phage VGs and
VGr adsorbed to susceptible and resistant
germlings, respectively, and specific adsorption leading to host lysis,
which is modeled as an infection event (rate l) after
nonspecific adsorption. This produces a replicating phage state in an
infected host I. Lysis occurs at a rate , releasing
b free-phage particles. In a model extension, lysogeny is
also included as an outcome of infection. Host aging and
differentiation transfer adsorbed phage between compartments following
host changes. Thus, resistance can be acquired before infection by
nonspecific adsorbed phage.
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The heterogeneity of the colony structure was also reflected in the
phage dynamics. Phage occurred in six states: a free state Vf, replicating phage within an infected host
propagule I, or adsorbed on the surface of the available
hyphae, i.e., adsorbed to susceptible and resistant substrate mycelium
(VTs and VTr) and
susceptible and resistant germlings (VGs and
VGr) (Fig. 1). We excluded lysogeny because its
low frequency in our experiments implies lysogeny does not have a
significant affect on the growth cycle dynamics.
Experimentally, we measured the number of viable spores, total
propagules (T), and free phage (Vf).
Spores, germlings, and substrate mycelia were assumed to contribute
equally to the propagule count, and phage lysis was assumed to remove a
propagule. A model with differential contributions of spores and
mycelia to the total propagule assay also was examined to see if this
assumption affected the fit to the data.
A simulation of the mathematical model is shown in Fig.
2 that demonstrates four key features of
the model. (i) Phage growth depends on susceptible propagule numbers.
Phage growth is initially rapid since susceptible germling density is
high after spore germination, but it declines as resistance is
acquired. A second phase of phage growth can occur if the host produces
a high density of susceptible tips, Ts, on day 3 of the stimulation, as indicated by the rise in phage adsorbed to
susceptible hosts. (ii) Phage adsorption to substrate mycelia protects
young tips from infection. Nonspecific adsorption of phage during the
vegetative phase produces a decline in the free phage density (Fig. 2,
day 3) even though the total phage level increases through the lysis of
substrate mycelia. Free-phage density reduction protects young hyphae
from infection since phage adsorbed to resistant mycelia are not
infectious unless they reenter the free-phage pool by desorption (Fig.
1). This explains why although susceptible hosts (young tips) are in a
10-fold-higher density at day 4 than at day 0 they do not induce
significant phage growth. (iii) Temporary cessation of growth occurs
when the vegetative capacity is achieved. The increase in total
propagule numbers temporarily ceases (Fig. 2, days 5 and 6) prior to
the appearance of spores. Growth cessation has been observed
experimentally (13, 26). (iv) Differentiation of
germlings into substrate mycelium does not correlate with resistance
acquisition. In this simulation, differentiation of germlings is slow,
whereas the acquisition of resistance by germlings is rapid. Our data
suggest that these time scales are in fact similar, a result that is
not due to the linking of these effects in the model.

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FIG. 2.
Model simulation. (A) Host dynamics: spores
(   ), susceptible germlings
Gs (-----),
susceptible mycelia Ts
(·······),
resistant germlings Gr
(-·-·-)
and resistant mycelia Tr (  ). (B)
Phage dynamics: free phage Vf (  ); phage
adsorbed to susceptible hosts, Vs = VGs + VTs
(----); and phage adsorbed to resistant hosts,
Vr = VGr + VTr
( - - ). A sporulation cycle is included
to demonstrate the increase in total propagule number after the
cessation of exponential growth of the mycelia. Sporulation is modeled
as a timed event from germination (18). The parameters in
this simulation were chosen to emphasize the model properties discussed
in the text: µ = 3 day 1, K = 4 × 106 CFU g 1, k = 1
day 1, Pd = 0.01, b = 300, + = 100 day 1
CFU 1 g,  = 1 day 1,
l = 2 day 1, G = 50 day 1, T = 2 day 1, = 25 day 1, = 0.12 day 1, and g = 6 day 1.
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MATERIALS AND METHODS |
Sterile, unamended Warwick soil (32) was inoculated
with Streptomyces lividans spores (TK24) and phage (KC301)
in two protocols. In experiment 1, 1.6 × 106 CFU of
TK24 g
1 and various amounts KC301 were used as follows:
microcosm 1A, 1.3 × 104 PFU g
1;
microcosm 1B, 1.3 × 103 PFU g
1;
microcosm 1C, 1.3 × 102 PFU g
1;
microcosm 1D, 1.3 × 101 PFU g
1; and
microcosm 1F without KC301. In experiment 2, 2.0 × 104 PFU of KC301 g
1 and various amounts of
TK24 were used as follows: microcosm 2A, 2.0 CFU g
1;
microcosm 2B, 2.0 × 101 CFU g
1;
microcosm 2C, 2.0 × 102 CFU g
1;
microcosm 2D, 2.0 × 103 CFU g
1;
microcosm 2E, 2.0 × 104 CFU g
1;
microcosm 2F, 2.0 × 105 CFU g
1; and
microcosm 2G without TK24. KC301 is a derivative of
C31 and contains a thiostrepton resistance gene (8).
Sterile soil was prepared by autoclaving twice at 121°C for 15 min
and then checked for sterility prior to use by plating on nutrient agar
(Oxoid) for 30 days at 28°C. Inoculants were mixed with sterile
distilled water to obtain
67-kPa matrix potential. The microcosms
were incubated at 22°C for up to 15 days with loosened lids to
facilitate gas exchange. No detectable moisture loss occurred during
this period.
Measurements (destructive sampling) of total streptomycete propagules
(16), spores (16), free phage (21),
lysogens, and lysogenic spores were obtained 0, 1, 2, 5, and 15 days
after inoculation. Lysogens were detected via thiostrepton resistance. Separate microcosms were prepared for each sampling day and for each
extraction type. The microcosms consisted of 20 g of soil for the
phage assay, 10 g of soil for assaying total propagules, and
100 g of soil for assaying spores. Triplicate platings were taken
from two microcosms for spore measurement and from three microcosms for
total propagule and phage assay. The lower limits for detection of
phage and total propagules were 13 PFU and 20 CFU/g of soil,
respectively. Two experimental protocols were used, varying either the
phage inocula or the spore inocula (see above). These experiments were
performed at different times of the year, with different phage, spore,
and soil batches, although all batches originated from the same phage,
spore, and soil stocks. These data have been partially discussed
previously (25), and the extraction methods are also
discussed elsewhere (23).
The burst size and rise time were determined by performing one-step
growth experiments according to the method of Lomovskaya et al.
(22). In brief, phage lysate was added at a multiplicity of
infection of 0.1 to a suspension of TK24 and incubated at 30°C for 30 min (to achieve maximum phage adsorption). Antiserum was added to
neutralize the phage, and the suspension was diluted by a factor of
1,000 and assayed for PFU at specified times.
Statistical significance is based on analysis-of-variance and Student
t tests.
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RESULTS |
Streptomycete growth dynamics.
We monitored a single
streptomycete growth cycle (Fig. 3).
Germination was complete by day 1, vegetative (exponential) growth occurred during days 2 to 5. Sporulation began during days 2 to 5, and
by day 15 the growth cycle was complete. The final total propagule
counts of microcosms 2B to 2F were 3 × 107 to 6 × 107 CFU g
1; microcosms 2D, 2E, and 2F were
not significantly different (P > 25%), as were
microcosms 2B and 2C (P > 10%). The total propagule count decreased significantly at day 1 (P < 1%) to
approximately 10% of the initial value, with significant growth in the
next 24 h (P < 1%). This fall occurred in the
absence of phage (microcosm 1F).

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FIG. 3.
Growth curves (log10) for experiment 1 (solid lines) and experiment 2 (dashed lines). (A) Spore counts. (B)
Total propagules. (C) Phage counts (microcosms 2A, 2B, and 2C have less
growth than microcosm 2D and are omitted for clarity). (D) Lysogen
counts. For experiment 1, an average over microcosms is shown for spore
and total propagules since streptomycete growth is identical across
microcosms (P > 1% for microcosms 1A, 1B, and 1D).
Typical error bars (95%) are shown as indicated, displaced to the
right for clarity. Their skewed appearance is due to the logarithmic
scale; the confidence intervals were computed based on the absolute
values. Symbols (A and B): 2A, ; 2B, +; 2C, ; 2D, ×; 2E, ;
2F, * with a dashed line; experiment 1 (average over microcosms),
solid line. Symbols (C and D): 1A, ; 1B, + (experiment 1, solid
line); 2D, ; 2E, ×; 2F, (experiment 2, dashed line). Data are
reprinted from Gene Transfers and Environment
(25) with permission from the publisher.
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All microcosms (Fig.
4) showed identical
relative growth following inoculation at days 1 and 2 (
P > 5%), even though the phage
count varied by 3 logs (Fig.
4).
Thus,
S. lividans growth is independent
of the phage at
these inoculation densities, and the decrease
in the total propagule
count over the first 24 h cannot be attributed
to either phage
lysis or to a crowding effect (
31). At day 5,
the relative
growth was significantly different between microcosms
(
P < 10
14; microcosms 2D, 2E, and 2F), although the total
propagule counts
were not identical either (
P = 3 × 10
6). The relative differences were significantly
reduced by day
5 from an initial scaling of 10 between microcosms 2C,
2D, 2E,
and 2F to 1.3, standard deviation [SD], 0.02 (best fit),
indicating
that exponential growth had ceased by this time. Thus, there
is
a weak dependence on the initial inoculation density in the total
propagule count at day 5. However, microcosms 2D, 2E, and 2F were
in an
identical state of sporulation by day 5 (
P > 20%). We
attribute
differences in growth between microcosms over the first
48 h solely
to different inoculum levels, but during the
subsequent 3 days
of vegetative growth the microcosms all reached the
same density
and stage in the growth cycle to a fair approximation.

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FIG. 4.
Plot of total propagule growth relative to the inoculum
against time on a log10 scale. Microcosms 2C to 2F and an
average over microcosms for experiment 1 (adjusted for the difference
in extraction efficiency) are shown. Symbols: 2C, ; 2D, +; 2E, ;
2F, ×; experiment 1, .
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The total propagule count increased over days 5 to 15 by three- to
eightfold (Table
1). This increase is
caused by the increase
in the spore count. In experiment 2, spores
contributed 11% of
the total propagule count at day 5 and 93% on day
15 (Table
1).
In experiment 1, the spore contribution to the total
propagule
count at day 15 was low (12%), perhaps due to a crowding
effect
suggested by the poor gain in spores during the growth cycle
(Table
1).
Since the microcosms all reached the same state of growth at day 5, the
exponential growth phase ended by reaching a saturation
capacity prior
to day 5. This saturation capacity is the vegetative
capacity
(
K) of the mathematical
model.
Phage growth dynamics.
Phage growth was dependent on the state
of S. lividans. During the first 24 h, a large increase
in phage density occurred for the higher streptomycete inoculum
microcosms (Fig. 3C), was constant for 24 h, and then decreased
dramatically in all microcosms between days 2 and 5. Day 5 and 15 counts were equal, indicating that the interaction was complete and
that spores were not interacting with phage. Phage growth during the
first 24 h in experiment 1 was poor compared to that expected from
the trends in experiment 2 (Fig. 3C). In the absence of host, the phage
count gradually declined as phage particles were inactivated or became
unavailable for detection by the assay (not shown). These data suggest
that phage may be adsorbed by the mycelia, similar to the adsorption observed in liquid culture (22, 30). The phage assay detects only unadsorbed phage because of the gentle extraction process (23). Therefore, phage adsorption caused the dramatic
decrease in phage count over days 2 to 5 correlating with the increase in mycelial density.
Since the increase in phage numbers occurs within 24 h of
inoculation the number of germinated spores lost through lysis can
be
estimated as (
Vi
V0)/
b for a
burst size
b, where
Vi denotes
free
phage density at day
i. The loss of host propagules can be
compared directly to the number of available host propagules at
day 0,
Sinoc, the inoculation density. For a burst size
of 120
(see below), effectively all propagules would be lysed for
microcosms
2E and 2F ([
Vi
V0]/
bSinoc values estimated as 71%, SD
21% and
110%, SD 12%, respectively). Such high losses through phage
lysis
would dramatically affect host growth and should produce effects
similar to those seen in liquid culture, where the bacteria can
be
eliminated (
4). However, the growth of the host was
unaffected
by the presence of phage (Fig.
4), suggesting that phage
growth
resulted from lysis of only a small fraction of the host
propagules.
Lysogeny.
Throughout these experiments the lysogen counts were
low, indicating that lysogens were a minority (<1% of host
population) and that lysis was the more common outcome of infection.
Liquid culture.
The burst size for KC301 on TK24 hosts was
120, standard error of the mean (SEM) 6. This is comparable
to
C31 and
A7 with burst sizes of 10 to 80 (22,
23) and 70 to 100 (11), respectively. The rise time
(i.e., the time from addition of antiserum to the end of phage
increase) was 60 min.
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MODEL APPLICATION |
Basic model.
We estimated the growth and interaction
parameters for the model schematically described in Fig. 1. Sporulation
was excluded because we could not estimate the rate of this process
from the data set. This restricts analysis to days 0 to 5, which are
independent of the sporulation cycle. We initially restricted modeling
to microcosms 2B to 2F. Microcosm 2A was removed because of its very low inoculum level. The number of datum points per microcosm is low
(measurements were only made at days 0, 1, 2, and 5), but these data
are sufficient since the doubling time of the streptomycetes is
expected to be 6 to 16 h, although rapid changes in the first 24 h may have been missed. The availability of multiple microcosms with various inoculation conditions ensures model validity over a wide
range of initial conditions.
We first developed a "basic model" that (i) ignored lysogeny, (ii)
assumed that substrate mycelia were resistant to phage
lysis
(
11), and (iii) assumed that the decrease in the propagule
count at 24 h resulted from a failure of germlings to
differentiate
successfully. Modifications and extensions to this model
were
then
examined.
Determination of parameters.
Extraction efficiencies were
estimated from day 0 measurements (Table 1). Three parameters
the
germination rate (g = 6.0 day
1), the
lysis rate of infected host propagules (
= 1.0 h
1), and the decay rate of free phage in soil (
= 0.12 day
1)
were estimated directly because they
determine an effect that is either very rapid or very slow and
therefore they are not significantly correlated with the other
parameters (verified by alteration of these values over reasonable
ranges [data not shown]). The germination rate was estimated by
comparing the spore counts on day 1 with those on day 0 by the formula
g =
loge
(S1/S0) (Table 1), which models
germination as a probabilistic event with an exponential distribution.
The decay of free phage was estimated from microcosm 2G (data not
shown), and the lytic time period was estimated from the liquid culture.
The nine remaining parameters were estimated by optimizing the fit of
the model to the data using a sum-of-squares statistic
denoted "SS"
(see
Appendix and reference
29). This method uses
the 29 datum points (day 1, 2, and 5 measurements) to simultaneously
estimate all nine parameters. The SS was minimized in the
nine-dimensional
parameter space, i.e., the total error between
observed and model
predictions of the total propagule and free phage
counts summed
over days 1 to 5 was minimized. The incline of SS away
from that
minimum determines the parameter confidence intervals. The
burst
size
b was treated separately from the other
parameters (see below).
The best fit of the basic model to experiment 2 is shown in Fig.
5 and
6, with the parameter estimates in Table
2. The only strong
correlations in the
parameters (correlations with
b were not determined;
see
below) were between µ, and
Pd (
r =

0.869) (Fig.
7), between
G with
+ (
r = 0.633), and between
G and
l
(
r = 0.581). All other parameters were weakly
correlated
(
r < 0.35). The parameters are discussed in
turn below.

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FIG. 5.
Fit of basic model to total propagule data of experiment
2, microcosms 2B to 2F. The data are time displaced for clarity. Error
bars are 95%. The parameters are given in Table 3. Note the uniformity
in the growth over the first 3 days, which reproduces the scaling
behavior of Fig. 4. Symbols: 2B, (  ); 2C, + (   ); 2D, (-----); 2E, × (-----); 2F, ,
( - - ).
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FIG. 6.
Fit of model to phage data for microcosms 2B to 2F.
Symbols: 2B, (  ); 2C, + (   ); 2D,
(----); 2E, × (------); 2F, ( - - ).
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FIG. 7.
Correlation between parameters
Pd, the probability of a germling
differentiating successfully, and µ, the mycelium growth rate. The
results are based on 2,000 Monte Carlo simulations. The 90% confidence
intervals of the projected distributions are shown. The joint 90%
confidence interval calculated from the SS lies inside these separate
confidence intervals.
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Burst size (b).
A good upper bound for the burst
size could not be determined from this data set because streptomycete
growth was independent of phage density. Thus, although SS decreases as
b increases from 100 to 300, it plateaus over the range
b = 300 to 1,000, where SS would normally have a
valley. This prevents traditional estimation of b. We fixed
the burst size at b = 300, a value equal to that in the
first minimum, and derived estimates and confidence intervals of the
other parameters subject to this constraint. A lower confidence bound
for the burst size was then determined: b > 150 (90%
confidence; see Appendix for details). Liquid culture measurements
suggest that the burst size is 120; however, a burst size this low is
inconsistent with our data set (Table 2).
Colony formation (µ, K, Pd,
k, and
G).
The vegetative
capacity estimate agrees with the day 5 total propagule count for
microcosms 2D, 2E, and 2F. We predict that at this time these
microcosms had ceased growth. The growth rate µ corresponds to a
doubling rate of 5.5 h. The probability Pd of a germling forming a colony was less than 1%, i.e., most of the
germlings failed to produce successful colonies. Resistance to phage
lysis was attained at the same rate as differentiation,
G ~ k, suggesting that acquisition of
resistance might be associated with exponential growth and changes in
the early colony structure. This similarity of time scale means that
most germlings were available for lysis, and only later did a
proportion (of those that escape lysis) successfully form colonies. The
ability of the model to satisfy the lack of an impact of the phage on the host population is particularly apparent in microcosm 2F, where ca.
50% of the inoculum was lysed, and 1% of those remaining developed
into colonies. In the absence of phage, the total propagule counts
would have doubled at days 1 and 2, a change that could not be detected
given the measurement errors.
Phage infection (
± and l).
The
rate-limiting step for phage infection (two-step process
[1]) changed with the host density from adsorbtion to
phage entry. Adsorption to mycelia was rate limiting for total
propagule densities of <105 CFU g
1, 3%
(ratio l/
+) of the vegetative capacity
K (microcosms 2A to 2E). In microcosm 2F the rate of phage
infection was primarily limited by phage entry after adsorption to the
surface (Fig. 1). Liquid culture estimates of the adsorption constant
+ are 2 × 10
10 to 8 × 10
10 ml min
1 (1, 11, 22). By
converting to an effective volume of water (equating
67-kPa matrix
potential with 15% volume to weight), we calculated
+
to be 2 × 10
9 ml min
1 from our data.
The similarity of these values is consistent with our interpretation of
the phage-host interaction.
The SS for this basic model has a probability of about 0.01%. This low
value was caused by high contributions to SS from two
points: microcosm
2B (phage on day 1) and microcosm 2E (phage
on day 2), suggesting that
these data are outliers. Excluding
microcosm 2B or 2E reduced the SS to
30 (
P = 1.2%) and 31 (
P =
0.9%),
respectively; removal of both gave an SS of 13 (
P > 16%).
Variations on the basic model.
We analyzed four extensions of
the basic model in which some of our original assumptions are relaxed.
(i) Modification of saturation dynamics.
In the basic model,
growth rate saturation was modeled as logistic, µ[1
(M/K)], which can be interpreted as inhibition of growth by mass
action effects, e.g., secretion of an inhibitor with high diffusivity
and inhibition proportional to the local concentration of the
inhibitor. However, growth is probably correlated over a colony,
suggesting inhibition of a more general form, µ[1
(M/K)
]. As discussed in Results, the vegetative
capacity also may depend on inoculum through a scaling behavior
K ~ AS0
(Fig. 3B). These
modifications lead to a (nonsignificant) reduction of SS to 46 (with a
best fit for
= 3,
= 0.05). Thus, the exact form of
the host growth dynamics is not critical in modeling these data.
We analyzed data from both experiments together with these
modifications, attributing differences in phage dynamics between
experiments to a difference in burst size and differences in vegetative
capacities to a weak dependence on the initial inoculum. The fit
was
very poor (
P = 10
8, SS = 115 with a
contribution of 80 from experiment 2, 38 degrees
of freedom),
suggesting that the model can adequately describe
either data set alone
but cannot explain both data sets with all
parameters identical except
for burst size. We hypothesize that
differences between these
experiments are due to differences in
phage adsorption rates and
infection cycle
dynamics.
(ii) Substrate mycelium susceptibility.
In the basic model,
germlings could age but substrate mycelia were assumed to be resistant
to phage lysis even though hyphal tips are probably susceptible to some
extent (11, 22, 30). We added a parameter,
T, for the rate of resistance acquisition by
substrate mycelia and estimated the 10 parameters of Table 2 as before.
Germlings became resistant at rate 1.3 day
1, independent
of the value of
T. For a
T value as low as 50 day
1 there
was no appreciable change in the goodness of fit (SS = 54). Below
this value, lysis of substrate mycelium and total phage in the system
increase as the
T decreases. For a
T value of >50 day
1, the phage
lysis of germlings dominated. Lysis of substrate mycelia became
important as the
T decreased to 30 to 50 day
1 (Fig. 8). For a
T value of >80 day
1, the free
phage at day 5 constituted 2.5% of the total phage, whereas at
T = 25 this fraction was 1%. Thus, phage derived from the lysis of substrate mycelia were adsorbed, while the
quantity of phage produced by germling lysis remained relatively constant. A lower confidence limit on
T
(90%) was 29 day
1, corresponding to a susceptible
half-life of 35 min. The important parameter for measuring
susceptibility of hyphae to phage lysis is the ratio of half-lives
T/
G, estimated to be >30 at a
90% confidence level. This result suggests that the phage-hypha interaction depends on the state of the colony. Identical results were
obtained by varying the rate constant l, i.e., substrate hypha exposure
T
1lT was at
least 30 times less than the germling exposure
G
1lG (90% confidence).

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|
FIG. 8.
The proportion of phage that originated from lysis of
substrate mycelia as a function of the aging rate
T in units per day. Microcosms 2B to 2F are
shown in decreasing sequence, i.e., 2B (  ), 2C
(   ), 2D (----), 2E
(·······), and
2F (- - -). Germlings acquired resistance
at a rate G that remained approximately
constant at 1.3 day 1. In microcosm 2B, the phage growth
was so low that changes in numerical accuracy of simulation are
apparent at a T of 100 day 1
compared to surrounding points.
|
|
For a
T value of 50 day
1, a
hyphal tip is susceptible for only about 20 min compared to 18 h
for germlings. During
exponential growth, the fraction of the colony
that was susceptible
is µ/
T, with a value
of ca. 6%.
(iii) Lysogeny.
We assumed a constant probability of lysogeny
per infection, a spontaneous reversal rate of zero, and that the
extraction efficiency for the lysogens was the same as that of the
total propagules. Under these assumptions the probability of lysogeny was 2 × 10
4, with a 90% upper confidence limit of
5 × 10
4 compared to a frequency of lysogeny of
C31 observed in liquid culture of 30 to 40% (22). The
low frequency of multiple infection of hyphae predicted by the model
for these soil experiments probably explains this difference and is
consistent with an environmental dependence of the lysis-lysogeny
switch (17).
(iv) Models for propagule loss after germination.
In the basic
model, the decrease in total propagule count during the first 24 h
was attributed to germlings failing to form colonies. Two alternative
hypotheses are that not all spores form viable germlings
(Pg < 1; Fig. 1) or that spores,
germlings, and substrate mycelia contribute unequally to the total
propagule count. We quantified the second alternative as:
where
eT is the assay efficiency (as
measured on spores at day 0) and
G and
T are the relative assay
efficiencies for
germlings and total propagules,
respectively.
The statistic SS indicates that these two models are not significantly
better at describing the data (SS = 51 and 49, respectively).
Again significant contributions to SS came from two or three outliers.
The SS plateaued in burst size at 400 and 200 for the two models,
respectively. Parameters that could be suitably compared lay within
the
confidence intervals of Table
2. Therefore, our estimates
are robust
against the as-yet-unknown process causing total propagule
loss during
the first 24 h. Possible explanations are a 99% failure
of
germlings to differentiate into viable mycelia, failure of
55% of
spores to establish a colony on germination, or a 5:2 efficiency
ratio
for detection by the assay for spores and mycelia (or
germlings).
 |
DISCUSSION |
Our three main observations were a large burst size (Table 2), a
lack of impact of the phage on host growth (Fig. 4), and a high
susceptibility to infection of germlings relative to young substrate
mycelium (Table 2 and Fig. 8). The difference in the burst size
estimates relative to liquid culture can be explained by environmental
dependence (28), and molecular explanations for differing
susceptibilities and adsorption have been proposed (6, 12).
However, these factors also can be explained by spatial effects:
spatial colony heterogeneity, localized modification of the environment
by hyphae (19), and the spatial distribution-correlation of
phage and hosts throughout the microcosm. Liquid culture destroys these
spatial effects because of high diffusion and mixing, while growth on
agar reduces these effects by restricting growth to the colony
boundary. At the molecular level, phage adsorption may be affected by
spore and hyphal modification of their local environment. For example,
water absorption by the spore could localize phage to germlings, and
slow diffusion of phage relative to colony growth will produce high
local concentrations of phage after lysis and reduce the effect of
phage relative to the total amount of phage present. Local adsorption
of phage by substrate mycelia protects substrate hyphal tips more than
it does germlings and could partially explain the increased
susceptibility of germlings to phage lysis relative to the substrate mycelium.
There are two biological uncertainties in this system: the identity of
the adsorbing material and the quantification of mycelial propagules.
Because of the physical separation of the aerial mycelium from the
substrate mycelium, the substrate mycelium is likely to be the
adsorbing material (32), as assumed in the model. However,
since adsorption is only important as the mycelial mat matures, the
dynamics would be mathematically similar and the exact identity of the
adsorbing material is not crucial for parameter estimation. The
mycelial nature of streptomycetes is potentially problematic,
principally because 1 CFU need not be a lytic unit. However, this
problem does not affect parameter estimation since phage growth is
restricted to the first 24 h and the streptomycetes are in
discrete lysable units during this time because of the absence of septa
(20). Further, differential contributions of spores and
mycelia to the total propagule assay cannot explain the data any better
than can alternative models.
Our analysis implies that the qualitative form of the streptomycete
growth cycle and phage-streptomycete interactions observed in liquid
(11) and agar plates (7, 18) can explain the dynamics in soil but that both the soil environment and colony heterogeneity are important variables. We note, specifically, the
following points. (i) Vegetative exponential growth stops after
reaching a vegetative soil capacity, at approximately 10% of the final
soil capacity, prior to the sporulation cycle. (ii) Phage do not
significantly affect streptomycete growth. (iii) Phage propagation on
germlings is more successful than on developed colonies. Thus, mycelial
susceptibility to phage lysis varies with age (11, 22, 30).
(iv) Adsorption of phage to mycelia significantly reduces the density
of free phage. Adsorption dominates the phage dynamics during the
vegetative phase of the host, reducing free-phage density by a factor
of 50 relative to the total phage in the system. (v) There is a
phage-independent growth pause of the host during the first 24 h
and a significant decrease in the total propagule count at 24 h.
This decrease can be explained by either a failure of 55% of spores to
establish a colony on germination, 99% of germlings failing to produce
viable mycelia, or a 5:2 efficiency ratio for detection of spores and
mycelia (and germlings), respectively, in the total propagule assay.
(vi) The burst size is large, with a b of >150 (90%
confidence) and a best estimate of b of 300 (germling
differentiation failure model).
These results emphasize the role of the environment in the growth and
interaction characteristics of streptomycetes and phage. However, in
contrast to previous work highlighting the importance of the
environment in affecting burst size (15, 28) and the lysis-lysogeny switch (17), which can be explained through
the nutrient status of the host, our analysis suggests that physical processes within the environment (e.g., diffusion) significantly affect
ecosystem dynamics. Further experimental work is required to clarify
the contribution of the environment to the dynamics with regard to
physical processes and nutrient status. Experiments incorporating in
situ monitoring of DNA for phage (9) and streptomycetes would also enhance the analysis and contribute to model development. In
particular, these methods could be used to test model predictions, for
instance, the ratio of free phage to total phage in the microcosm at
day 15 (estimated to be 1 to 3%) and the rate of decline of free phage
over the vegetative phase, predicted by our models to be equal to the
growth rate of the adsorbing medium.
 |
APPENDIX |
Mathematical model. The basic model schematically
represented in Fig. 1 consists of 14 coupled ordinary differential equations. The model parameters are listed in Table 2.
Susceptible Gs and resistant
Gr germlings have dynamics described by:
|
(A1)
|
and
|
(A2)
|
In equation A1 the terms are the creation of
susceptible germlings by germination (rate
g),
differentiation into substrate
mycelia at rate
k, infection
by adsorbed phage
VGs, and acquisition
of
resistance at rate
G, corresponding to the
first
term of equation A2. Resistant germlings differentiate at rate
k, the second term in equation A2. Germination reduces spore
numbers
as
e
gt. Germination is successful with
probability
Pg.
Substrate mycelia occur in four states: susceptible mycelia
(Ts), resistant mycelia
(Tr), an intermediate state
(Ti; not shown in Fig. 1), and nonviable
mycelia (Tfail). The last two states are
introduced to ensure that germling differentiation and aging are
independent processes (i.e., to prevent parameter correlations) and to
prevent adsorbed phage release to the environment on differentiation
failure, respectively. The intermediate state
Ti is differentiated (giving rise to
growing tips) but acquires resistance on a germling time scale
G. Tfail models
the fact that failed germlings present an adsorbing surface for a
period of time. Decay of this adsorbing surface is not included since
the surface area is insignificant once exponential growth is underway,
i.e., within 24 h. The substrate mycelium dynamics are as follows:
|
(A3)
|
|
(A4)
|
|
(A5)
|
and
|
(A6)
|
Here
M =
Ts +
Tr +
Ti is the total
growing mycelia with a growth rate µ(
M) = µ(1
M/
K). The terms in equation A3 are the production
of susceptible
mycelia by growth, the loss by infection by adsorbed
phage
VTs, and the acquisition of resistance at rate
T.
For resistant mycelia, equation A4, the
terms are differentiation
from resistant germlings and the acquisition
of resistance by
the intermediate state and susceptible mycelia.
Similarly, equations
A5 and A6 record the production and loss of
Ti and
Tfail.
The phage compartments consist of free phage
Vf, replicating phage in an infected host
I, and phage adsorbed to the host compartments above,
denoted VGs,
VGr, VTs,
VTr, VTi,
and Vfail. The phage dynamics are as follows:
|
(A7)
|
|
(A8)
|
|
(A9)
|
|
(A10)
|
|
(A11)
|
|
(A12)
|
and
|
(A13)
|
Phage adsorption kinetics are based on mass action. The first two
terms in equations A8 to A13 represent adsorption and desorption
and
correspond to the third and fourth terms of equation A7. Adsorbed
phage
compartments mirror aging, differentiation, and infection
of the
underlying host equation, except for an extra term at infection
that
models the additional phage adsorbed to the surface of the
hypha at
infection. The number of additional particles adsorbed
per propagule
upon infection is given by
sGs =
VGs/
Gs and
sTs =
VTs/
Ts from Poisson statistics for
germlings and susceptible substrate
mycelia, respectively. These phage
particles are released to the
free compartment upon infection. Under
our experimental conditions
this refinement is not important since
infected propagules tend
to have very few adsorbed
phage.
An infection event results in concurrent loss of a host propagule
(e.g., the third term in equation A1), the loss of an adsorbed phage
particle, and the creation of an infected host I, as
follows:
|
(A14)
|
Phage replication produces
b free-phage particles per
infection event on lysis of the infected host at rate

, the first
term of equation
A7.
Lysogeny can be added by introducing a probability of an
infection event leading to lysogeny. This gives rise to a lysogen compartment L and adsorbed phage VL.
Alternative growth models for filamentous organisms can be found
in references 27 and 34.
Initial conditions. All germling and substrate mycelium
compartments are initially empty. The growth process is initiated by
germination from spores as calculated in equation A1. Initially, free
phage is set to the inoculum level, and all other phage compartments are empty.
Parameter estimation. We use a standard sum-of-squares
statistic (SS) for estimation of the model parameters, summing over the
observables (phage, total propagules, and lysogens [optional]); over
microcosms; and over days 1, 2, and 5. The time points are independent
because of destructive sampling. The measurement errors are estimated
for each time point from multiple measurements and are likely to be
normal (deriving from Poisson statistics for plate counts). Thus, SS is
2(n
m) distributed (n
datum points and m estimated parameters). Parameters
,
, and g are fixed as discussed in the text, and SS is
minimized to estimate all of the remaining parameters concurrently. These parameters are initially set randomly, and repeat runs are performed from different random initial values to locate the global minimum. For the models considered, the SS has a minimum value of about
51 (experiment 2), which corresponds to P
0.018%.
We consider such values acceptable since the SS is the same order as
the 1% significance value of 38 on 20 degrees of freedom. This is
justified because there is evidence of outliers, and SS is sensitive to
measurement error underestimation that may derive from variation
between microcosms.
The nonlinearity of the model requires that SS be calibrated for
estimating parameter confidence limits. This is done through Monte
Carlo simulation (29). The 90% confidence intervals
calculated in Table 2 are performed on a Monte Carlo simulation of
2,000 points. This is sufficient, as shown in Fig. 7, since the points are well distributed across the confidence intervals. The 90% level
for the SS statistic is consistent with the approximation 
2(m) (confidence 1
, estimating
m parameters) for nonlinear models not far from linearity
(5). For eight parameters
0.12(8) = 13.4, while numerically we obtained 12.0. Throughout, significance intervals are projected onto the corresponding coordinate, i.e., the
90% significance value surface of the SS is identified and the lowest
and highest values of the various parameters for that surface are used
as the confidence intervals in Table 2. This is conservative given the
high dimension of parameter space and ignores all correlations between
the parameters (Fig. 7). Multiparameter significance intervals will be
narrower than the single-parameter estimates. For parameters that are
only constrained by the data in one direction, e.g., the burst size, we
fix these parameters at a suitable minimum and calculate the SS
statistic probability levels under these constraints. To obtain the
appropriate SS statistic for the full parameter space, we use the
2 distribution to adjust for a change in the degrees of
freedom, i.e., we normalize the SS to 93.1% on eight variables for
90% confidence on nine. These probability levels are reasonable
approximations for the full unconstrained probability distribution
since 
2(m) was a reasonable
approximation to the SS. This is equivalent to imposing a weak prior on
b.
 |
ACKNOWLEDGMENTS |
N.J.B. thanks J. Crawford for discussions on the spatial
effects in soil.
N.J.B. was supported by EPSRC Fellowship number B/94/AF/1822. P.M. was
supported by BBSRC grant number 88/FQS02672.
 |
FOOTNOTES |
*
Corresponding author. Mailing address: Mathematics
Institute, University of Warwick, Coventry CV4 7AL, United Kingdom.
Phone: 02476524682. Fax: 02476524182. E-mail:
njb{at}maths.warwick.ac.uk.
 |
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