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Journal of Virology, April 2001, p. 3121-3128, Vol. 75, No. 7
0022-538X/01/$04.00+0 DOI: 10.1128/JVI.75.7.3121-3128.2001
Copyright © 2001, American Society for Microbiology. All rights reserved.
Computational Analysis of Retrovirus-Induced
scid Cell Death
René
Daniel,
Samuel
Litwin,
Richard A.
Katz, and
Anna Marie
Skalka*
Institute for Cancer Research, Fox Chase
Cancer Center, Philadelphia, Pennsylvania 19111
Received 7 July 2000/Accepted 11 January 2001
 |
ABSTRACT |
It was shown recently that retroviral infection induces
integrase-dependent apoptosis (programmed cell death) in DNA-dependent protein kinase (DNA-PK)-deficient scid pre-B cell lines,
and it has been proposed that retroviral DNA integration is perceived as DNA damage that is repairable by the DNA-PK-dependent nonhomologous end-joining pathway (R. Daniel, R. A. Katz, and A. M. Skalka, Science 284:644-647, 1999). Very few infectious virions seem
to be necessary to induce scid cell death. In
this study, we used a modeling approach to estimate the number of
integration events necessary to induce cell death of
DNA-PK-deficient scid cells. Several models for
integration-mediated cell killing were considered. Our
analyses indicate that a single hit (integration event) is sufficient
to kill a scid cell. Moreover, the closest fit
between the experimental data and our computational simulations
was achieved with a model in which the infected
scid cell must pass through S phase to trigger apoptosis.
This model is consistent with the findings that
a single double-strand DNA break is sufficient to kill a cell deficient
in DNA repair and illustrates the potential of a modeling approach to
address quantitative aspects of virus-cell interactions.
 |
INTRODUCTION |
All cells are subject to DNA damage,
and unrepaired DNA damage can induce cell death. The extreme
sensitivity of some cells, such as those derived from the severe
combined immune-deficient (scid) mouse, led to the discovery
of genes and proteins that are required for DNA repair (41,
45). DNA-damaging agents induce a variety of lesions. For
example, ionizing radiation induces both single- and double-strand (ds)
DNA breaks (32). In contrast, UV radiation induces
primarily pyrimidine dimers (38, 44). The several types of
DNA-damaging agents differ in their potential to induce cell death
(32). The most lethal type of DNA damage appears to be an
unrepaired ds DNA break (32, 43). Analysis of the kinetics
of killing by DNA-damaging drugs or ionizing radiation indicates that a
single unrepaired ds break is lethal to both mammalian
(32) and yeast cells (3, 4, 20).
scid cells carry a mutation in the gene for the catalytic
subunit of the DNA-dependent protein kinase (DNA-PKCS),
which is a critical component of the nonhomologous end-joining (NHEJ)
DNA repair pathway in mammalian cells (6, 40). As a
consequence of this mutation, scid cells are hypersensitive
to DNA damage (5, 15). It was shown recently that
retroviral infection induces apoptotic cell death in scid
lymphocytic cell lines (10). The vectors used for those
studies do not express viral genes and are replication defective in
mammalian cells (avian sarcoma virus-derived) or have all viral coding
sequences deleted (human immunodeficiency virus type 1 derived). Thus,
contrary to a recent suggestion (7), viral gene expression
cannot account for this phenomenon. The scid cell killing
is, however, dependent on the presence of active, retroviral integrase,
the enzyme that catalyzes retroviral DNA integration (8, 13,
25).
The integrase-catalyzed DNA integration reaction proceeds in two
distinct steps. In the first step (processing), two nucleotides are
removed from the 3' ends of the linear viral DNA, and in the second
step (joining), these new 3' ends are joined to staggered phosphates in
both strands of host-cell DNA (8, 13, 25). The resulting
integration intermediate leaves single-strand gaps in the flanking host
DNA and unjoined 5' ends of viral DNA which must be repaired to create
a stably integrated "provirus." It has been proposed that apoptosis
is induced in scid cells because the integration event or
some other integrase-mediated activity is perceived as DNA damage that
cannot be repaired (10; Fig. 1).

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FIG. 1.
Model for integrase-dependent scid cell
killing. scid pre-B cells die by apoptosis when infected
with an integration-competent retrovirus (10).
(IN)n, retroviral integrase multimer.
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In those experiments, scid cells were infected at a
multiplicity of approximately two infectious virions per cell
(10). Despite this low virus-to-cell ratio, approximately
50% of scid cells died by apoptosis following retroviral
infection (10; Table 1). The
computational modeling approach described in this report addresses the
question of how many integration events are necessary to kill a
scid cell.
The models that were tested included variables relating to cell cycle,
because of its possible influence on both retroviral DNA integration
and induction of apoptosis. For example, it has been reported that
passage through mitosis is necessary for Moloney murine leukemia virus
(MoMLV) to enter the nucleus (36) and it is known that
MoMLV can replicate only in dividing cells. In contrast, the avian
sarcoma virus (ASV), which can also replicate only in dividing cells,
does not seem to require passage through mitosis to integrate its DNA
in target cells (22). However, it has been proposed that
ASV may need cellular DNA replication and, thus, a passage through S
phase for integration (21, 42). Therefore, although virus
replication is neither possible nor demanded in our experimental
system, cell cycle status may still be relevant to integrase-mediated
killing by the ASV-based retroviral vector used. In addition, in the
absence of DNA repair, passage through S phase and the attendant DNA
replication might cause single-strand gaps introduced during retroviral
DNA integration to be converted into highly lethal ds breaks (32,
43). Finally, expression of cellular proteins critical to
integrase-mediated killing may be limited to a specific phase of the
cell cycle. Thus, the cell cycle status of target cells was included in
our models.
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MATERIALS AND METHODS |
Computation.
All models were programmed in Fortran 77 and
run on a UNIX work station (DEC alpha). Model output was graphed using
Splus software. The Fortran source code can be obtained from S. Litwin at s_litwin{at}fccc.edu.
Infection protocols.
In the viability assays, pre-B S33
cells were infected as previously described (10). Log
phase cells were distributed in 24-well plates at 5 × 105 cells per ml per well. DEAE dextran at a final
concentration of 5 µg/ml and the ASV viral vector (IN+;
10) at a multiplicity of infection (MOI) of two infectious virions/cell were added to each well. The final volume was 2 ml per
well. The number of infectious virions was determined by the ability of
the vector to transduce a drug resistance marker after infection of
normal (DNA-PK-proficient) cells (10). Cell viability was
measured by trypan blue dye exclusion. At each time point indicated,
aliquots were removed from the individual wells and the number of
stained and unstained cells was determined (in samples of approximately
100) to estimate the percentage remaining viable. For infection at a
higher MOI (i.e., 5.4), 6 × 106 cells were pelleted
and then resuspended directly in the virus-containing medium, in the
presence of 5 µg of DEAE dextran/ml. The mixture was then distributed
into separate wells so that each contained 1 × 106
cells and the final volume was again 2 ml. Viability was measured as
described above.
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RESULTS |
Experimental design.
One goal of this study was to determine
the number of integration events required to kill a DNA-PK-deficient
cell. First, a series of infections was carried out using a known titer
of the ASV-derived viral vector, and cell viability was monitored at
given times thereafter. As the ASV vector cannot replicate in the
mammalian cells, the experiments measure the effects of only a single
cycle of integration, that of the infecting vector. The observed
pattern of cell killing was then compared to patterns predicted from
mathematical models that take into account a number of critical
parameters described below.
Parameters included in the computational analyses.
All of the
models developed for our analyses use the same method of determining
viral adsorption time. However, the models differ in the way cell cycle
status affects apoptosis timing after viral adsorption. Three
parameters are used to control this timing: (i) the delay time,
d1, between virus adsorption and
integrase-mediated joining of viral to host-cell DNA; (ii) the delay
time d2, the minimum time between the initiation
of apoptosis and detectable cell death; and (iii) the generation time,
, of target cells.
Delay
d1 includes the time required for viral
entry into the cell (after cell contact), reverse transcription,
nuclear import
of the preintegration complex containing viral DNA and
bound integrase,
and the processing and joining reactions mediated by
the retroviral
integrase (
8,
13,
25). After infection with
MoMLV, it takes
6 to 8 h for viral DNA integration to be detected.
This includes
the time necessary for the virus to adsorb to a target
cell (
35).
Experiments with ASV infection of avian cells
(A. M. Skalka, unpublished
observations) suggest that the time
necessary for ASV-based vectors
to integrate into host DNA following
infection is probably between
4 and 8 h. Therefore, intervals
ranging from 4 to 8 h were
considered.
The interval
d2 appears to depend on the
apoptosis-inducing agent. For example, dexamethasone-induced killing
has been detected
1.5 h after addition of the drug (
17).
We do not know the interval
needed for integrase-mediated killing.
However, it has been shown
that radiation treatment kills Ku-deficient
cells as early as
2 h posttreatment (
31). Thus, we have
incorporated a second,
adjustable, variable time interval into
our model, covering this
period. (See Fig.
3 legend for parameter
ranges.)
Detection of
scid cell death may be influenced by the
generation time of the cells. In the
scid cell line used for
these studies
(S33), the doubling time was close to 20 h under
optimal growth
conditions. However, this number differs somewhat from
experiment
to experiment, depending on the stage of the culture. In
addition,
the virus-containing medium added at the time of infection
can
slow the growth of S33 cells by as much as 20 to 30% (data not
shown). Generation time was thus included as another
parameter.
Structure of the model of infection of scid cells by
the retrovirus.
scid cells were suspended in growth
medium while in log phase. If we assume that scid cell
generation times are homogenous (29, 33, 34), then the
distribution of cell ages under these conditions is
where
a is cell age and

is generation time, here
approximately 1 day. Units of
a and

are hours. The age
distribution
has the property that there are always twice as many cells
of
age near zero as cells of age just short of

(Fig.
2, top). Our
simulation
model is based on an array of initial cells (
n = 1,000).
Times of birth of these cells start at


and end at 0. The set
of birth times is distributed in a nonlinear way so as to
closely
approximate the above age distribution (see Fig.
2, top). To
this
end we set the time of birth of the most recently born cell at
0 (
t1 = 0). Successive earlier birth times
t2,
t3, ... ,
tn are defined by
Approximately two infectious virions per cell were added to the
log phase cell culture at time zero. We model virus adsorption
as
taking place upon contact. All cells, alive or dead, may adsorb
viruses
in our model. Let
V be the concentration of free virus
in
solution,
C the concentration of cells, and
kV the rate constant
determining the rate of
viral adsorption by cells (
28). Then
describes the concentration of free virus over time. The
adsorption rate constant,
kV, is determined by
where
RC is the cell radius and
D is the viral diffusion constant given by
where
Rg is the gas constant,
T
is the absolute temperature,
N is Avogadro's number,

is
the viscosity of the medium, and
RV is the viral
radius. The virus and cell radii were determined
independently using
electron microscopy and represent the average
of five and six
measurements, respectively. Both are assumed to
be spherical in our
calculations. Parameters used were as follows:
RC = 0.5066 × 10
5 m;
RV = 0.573 × 10
7 m;
N = 6.0228 × 10
23 molecules/mol;
Rg = 8.315 × 10
7 ergs/mol
K;
T = 310 K; and

= 0.01005 P.

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FIG. 2.
Models for the age distribution of log phase cells, and
the relevance of cell cycle phase to retroviral DNA integration and
apoptosis in scid cells. (Top) The age distribution of cells
growing in log phase culture is a truncated exponential with twice as
many cells just born as there are about to be born (see text). The
simulation program starts with an inoculum of 1,000 cells whose birth
times are determined to closely adhere to this age distribution.
Illustrated is the process for a set of 50 cells. Each tick mark is a
cell age at the start of the simulation: the oldest cell is 24 h
of age and the youngest is 0 h. (A) Time line showing birth and
phases of the cell cycle and times of their occurrence.
tb, time of birth; s1 and
s2, start and end of S phase; , generation
time. The percentage of cells in S phase was determined by flow
cytometry analysis of propidium iodine-stained cells. We determined
s1 = 0.43 , s2 = 0.886 . The figures are not to scale. (B) Position of
replication fork at time t for tb + s1 < t < tb + s2. a,
fraction of genome replicated at time t; b,
fraction not yet replicated; a + b = 1. When t = tb + s1, a = 0, and when
t = tb + s2, a = 1. (C) If retroviral DNA
integration occurs prior to tb + s1, then the integration site is chosen at
random (uniformly) from the entire genome. Apoptosis will be signaled
when the replication fork intercepts the unrepaired integration site.
Even if integration occurs in S phase but the integration site is
(randomly) chosen beyond the replication fork, as illustrated, then,
again, apoptosis is signaled when the fork reaches the unrepaired
integration point. The chance of this event is b/(2
a + b) where b is the fraction of
the genome still unreplicated at the moment of retroviral DNA
integration. If t is the time of integration then
a = [t (tb + s1)]/(s2 s1) and b = 1 a.
Cell death is detected via trypan blue exclusion after delay
d2. (D) If viral integration occurs in S phase
but the site is selected from a branch of the already replicated
genome, then (absent other viruses) one daughter cell escapes apoptosis
while the daughter containing the unrepaired integrated site will
signal apoptosis when its replication fork reaches this site. The
chance of this type of integration is 2a/(2a + b). However, the infected daughter cell will signal
apoptosis at a time in her S phase that reflects the earlier integration event. For example, if the integration takes
place at t = tb + s1 + (s2 s1)/2, i.e., half-way through the genome, then
the chance that it lands on one of the already replicated branches is
2/3. Its position in the daughter cell genome is then randomly selected
between 0 and 1/2. Thus, the time of this daughter cell's apoptosis
will be uniformly distributed between tb + + s1 and tb + + s1 + (s2 s1)/2, rather
than uniformly over the whole of S phase.
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Between cell divisions, while cell concentration
C is
constant,
V(
t) =
V(0)
e
kVCt, where
t = 0 marks the start of such an interval.
V(t)/V(0) is
the
fraction of free viruses at the start of the interval that
remain free
at time
t. We identify this fraction with the chance
that a
randomly chosen virus free at
t = 0 remains free at
time
t. If
T is the adsorption time of this virus
then
p(
T > t) =
e
kVCt. If there are
nV free viruses, then the time,
Tmin, until one
of these is adsorbed,
diminishing their number to
nV 
1, has
exponential distribution
Following the results of Andreadis et al. (
1), we
account for the half-life of the amphotropic viral vector while in
solution
as 6.5 h, which we used throughout our simulations. When
a virus
was scheduled to infect a cell, we generated a deviate from the
exponential having this half-life. If the deviate was smaller
than the
elapsed time of the experiment at that point, the virus
was declared to
be inactivated. Otherwise it successfully infected
the
cell.
Time epochs are defined by intervals between cell births and between
viral adsorption events. New cell birth times are predetermined
by the
original birth order. A succession of random viral adsorption
times is
generated, according to the above distribution, where
each virus
adsorbed is assigned to a random cell. The cell stores
the exact time
of each viral adsorption and may be infected by
several (up to six)
viruses in the model. The sum of the time
intervals between viral
adsorptions is tallied and added to the
time of the most recent cell
division. When this tally exceeds
the time of birth of the next cell,
the last adsorption time is
discarded and computation is resumed after
the two new daughter
cells are added, the parent cell is removed, and
C is adjusted
accordingly. This exploits the
"forgetting" property of the exponential
distribution. The
simulation continues until the next cell birth
would occur beyond our
intended time horizon, here 36 simulated
hours.
Alternative models of scid cell killing by the
retrovirus.
Five models for cell killing by virus were considered
initially in fitting our experimental data (Table 1). Each assumes that
the trigger for apoptosis is retroviral DNA integration or some other
integrase-mediated event that takes place at a single locus. In what
follows, the triggering event will be referred to as "damage."
In model 1, cell cycle phase is not a critical parameter. The damage
occurs and apoptosis is signaled
d1 h after the
virus
contacts the cell, and cell death is detectable
d2 h thereafter.
If the interval
d1 is completed prior to the end of the cell
cycle
(see Fig.
2A), then cell death is detectable
d2 h later and the
infected cell does not
replicate. If cell division is completed
before interval
d1, then the two daughter cells randomly inherit
all infecting viruses. In that case the damage takes place in
a
daughter cell
d1 h after the virus infected the
parental cell,
and the daughter cell dies
d2 h
later.
In model 2, cell cycle phase is a critical factor. As ASV may require S
phase for integration (
22), this model stipulates
that
damage can occur only after the start of S phase. If delay
d1 terminates before S phase, then integration
and apoptosis commence
at the start of S phase. If
d1 terminates during or after S phase,
then
integration occurs at that moment and this triggers apoptosis.
When
delay
d1 terminates after the cell cycle is
completed, viral
hits are shared randomly by the daughter cells.
Daughters inheriting
the virus also require the start of S phase to
enter
apoptosis.
In model 3, damage can occur only at the end of the cell cycle (during
M phase) and death always occurs
d2 h later if
interval
d1 is completed before the end of the
cell cycle. During early
stages of mitosis, the nuclear envelope is
dissolved, which, as
already noted, is generally assumed to be required
for MoMLV DNA
and its integrase to gain access to host cell DNA
(
36). Otherwise,
damage is inherited as in models 1 and
2.
In model 4, apoptosis is signaled only when a cellular DNA replication
fork intercepts the damage during S phase (Fig.
2A
to D). In these
cases the damage is modeled to have taken place
randomly over whatever
nuclear material is present. Cell death
is detectable
d2 h after apoptosis is signaled. The amount of
nuclear material varies continuously from one to two genomes.
If the
cell's only damage occurs after S phase, this damage is
inherited
randomly by daughter cells (Fig.
2D). Such daughters,
again, signal
apoptosis only during their S phases. In this case,
as with model 1, one daughter will be damage free if only one
infecting virus entered
the parental cell or if all infecting
viruses damage the DNA of the
same
daughter.
A model in which integration is allowed only after the start of S phase
(as in model 2) but initiates apoptosis when the replication
fork
intercepts the damage (as in model 4) was also considered.
The behavior
of such a model is indistinguishable from that of
model
4.
In model 5, as in model 3, damage can occur only in M phase but
apoptosis can only be triggered in S phase. The initially
infected cell
does not enter apoptosis, and damage is randomized
to the daughter
genomes. The interception of a replication fork
with the damage in an
affected daughter cell is required to trigger
apoptosis. The daughters
whose DNA has been damaged fail to replicate,
and cell death is
detectable
d2 h after apoptosis
signaling.
Dead cells are also viral targets in all models and do not disintegrate
during the simulated experiment (36 h). Cells may
die from nonviral
causes. In the growing virus-free culture, a
constant fraction
(approximately 7%) of dead cells is observed.
In our models similar
results are obtained by setting a 6% death
rate for all cells at their
moments of replication. Two-hit options
are approximated from the
one-hit models in all cases by programming
the models to ignore the
first hit. Either the earliest infecting
virus (models 1, 2, 3) or the
one causing DNA damage closest to
but ahead of the replication fork
(models 4 and 5) determines
the time of cell death. Other viruses
infecting the same cell
have no effect other than to reduce the number
of free viruses
in
solution.
A single hit in model 4 provides the best fit to the experimental
data.
The left panels of Fig. 3 show
one- and two-hit least squares best fits with the data in Table 1 for
the five models described above. For model 1, the fit at 12 h is
achieved by delaying cell death approximately 12 h from viral
adsorption. Even so, the fits at 16, 20, and 24 h for one hit are
poor, as are the fits at 9, 24, and 36 h for two hits. For model
2, both one- and two-hit fits at 24 h are poor and the fit at
9 h for one hit and at 20 and 36 h for the two-hit option are
also poor. For model 3 the fit for one hit at 24 h misses the data.
This lack of fit is not sufficient, however, to reject the model (see
Discussion). However, the values for d2 (0.0 h)
are implausible, and the fits at 12, 16, 20, 24, and 36 h are poor
for two hits with this model. For model 4, the one-hit fit is good and
the parameters dictated are close to the predicted ranges. In contrast,
the two-hit fit is poor at 12, 16, 20, 24, and 36 h and the time
interval for d2 is not plausible. Finally, with
model 5 both one- and two-hit fits are poor at 12, 16, 20, and 24 h with implausible values for d2. In addition,
the fit at 36 h is poor for the two-hit option with this model.

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FIG. 3.
Five models for ASV integrase-mediated scid
cell killing. Each model is described in the text. Points represent the
experimental data in Table 1. (Left panels) Parameters ,
d1, and d2 were
determined to give least squares fits for all five models. Parameter
searches, however, were restricted as follows: 20 40; 4 d1 8; 0 d2 6 h. Solid lines represent
one-hit options; dotted lines represent two-hit options. (Right panels)
Five models at fixed delays d1 and
d2 with one- or two-hit options. In all cases
delay d1 is set at 4 h (lower curve),
6 h (middle curve), or 8 h (upper curve);
d2 is 1 h and = 22 h. Options
are represented as in left panels.
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We then examined the fit of all five models under conditions of fixed
delays
d1 and
d2. Delay
d1 was set at 4, 6, or 8 h,
which brackets
the range observed in vivo (
35; Skalka, unpublished
observation). Delay
d2 was set at either 1 (Fig.
3, right panels)
or 2 h (data not shown), which is consistent with
apoptosis induced
by either drugs or irradiation (
17,
31).
Generation time was
set at the average 22 h, which is a commonly
observed doubling
time for our log phase S33 cultures. We observed a
good fit for
the one-hit option of model 4 when
d1 was 4 h and
d2
was 1 h.
The fit was not as good with model 3 and poor for the one-hit
options of models 1, 2, and 5, regardless of the length of
d1 or
d2. None of the
models fit even remotely to the data when two-hit
options were
considered. We also examined the fits of models 3
and 4 when cells were
infected at a higher MOI, from the data
set provided in Table
2. Delays
d1 and
d2 and generation time

for fitting model 4 to the high MOI (5.4) data set were taken
from the least squares values
determined from the low MOI (2.0)
data set. Figure
4A shows that model 4 fits the high MOI
data
set without a change of these parameters. For model 3, however,
delays
d1 and
d2 and
generation time

were fit by least squares
directly to the high MOI
data set. Even so, the resulting fit
is poor and, moreover, requires
the unrealistic value of
d2 =
0.

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FIG. 4.
Further tests of models 3, 4, and a variant, model 6. (A) Model 4 at a high MOI (solid curve), using parameters derived from
the low MOI data set. Data points are from Table 2. Model 3 (dashed
curve) is a least squares fit. This best fit, nevertheless, fails at
the 12- and 36-h data points. (B) Least squares fit of model 6, a
variant of model 4. Each infecting virion releases integrase molecules
presumed to damage the host genome at multiple sites ( 50). Data
points are from Table 1. One-virion option, solid line; two-virion
option, dotted line.
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Finally, we considered a different scenario (model 6) in which
integrase molecules are released from an infecting virion and
the
nuclease activity of such molecules is capable of introducing
damage at
multiple locations in the host cell DNA. As each virion
contains
approximately 100 molecules of integrase (
8) and the
active enzyme is a multimer (minimally a dimer), we chose 50 as
a
reasonable minimal number of potential damage sites in model
6. In this
model the integrase molecules are released
d1 h
after
cell contact. As in model 4, apoptosis is signaled only in S
phase
when the replication fork encounters the unrepaired damage. If
the release of integrase occurs prior to S phase, then apoptosis
is
signaled very near the start of S phase. Apoptosis is signaled
very
soon after integrase release if it occurs in S phase. Release
of
integrase after S phase causes both daughters to inherit hits
and both
to signal apoptosis at the start of their S phases. If
the delay
d1 is completed after cell division, parental
viral
hits are randomly distributed between daughter cells. The results
(Fig.
4B) show a poor least squares fit of our data with model
6 with
either the one- or the two-hit
option.
 |
DISCUSSION |
We have used mathematical modeling to analyze the kinetics of
ASV-mediated scid cell killing and to evaluate the
importance of cell phase without the use of chemical or other blocks
that can introduce additional confounding variables. Our purpose was to
test several reasonable hypotheses of how viral infection leads to cell
death. In all models tested, two-hit versions are unequivocally refuted
by the experimental data. All but one of our one-hit models (model 4)
also fail to explain the data. The parameters in each model were
adjusted to provide the best fit possible (least squares) for that
model. Excepting models 3 or 4, no possible adjustment brings them into
conformity with the data. These failures are illustrated in Fig. 3 and
4 where model best fits widely skirt observations. Six independent
viability measurements were made at each sampling time. In three of the
four models there were two or three sampling times at which all six
viability values obtained were either above or below model predictions.
The chance of this event is p = 2
5 at
each sampling time. Model curves were forced to fit the initial sample,
at t = 0, hence only model fits at the seven additional sampling times were sensitive to parameter adjustment. The chance that
two or more sampling times exhibit this extreme asymmetry is given by
the binomial probability
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As a result each of the above models is rejected at this level of
significance, even though the number of sampling times
is fairly small.
This is noteworthy given the latitude in adjusting
model parameters and
the considerable data scatter at most sampling
times. Model 3 cannot be
rejected by our low MOI data; however,
it cannot be made to fit the
high MOI data. Model 4, on the other
hand, fits the high MOI data using
the same parameters (d
1, d
2,

) determined
from the low MOI
experiment.
Model 4 fits all of the existing data very smoothly, passing centrally
through the scattered viability measurements at each sampling time. It
does so using reasonable parameter values. There may be other models
that could be made to fit the experimental data equally well, but we
have not been able to find other alternatives that make biological
sense. All five unsuccessful models can now be set aside, having been
rejected by our limited data set. However, we claim only that our
phase-dependent model 4 is consistent with the data, not that it is
valid. Experiments of a different sort will be needed to refine or
reject this one remaining model.
The results of our modeling indicate that infection by a single
integration-competent virus is sufficient to induce scid
cell death. This interpretation is consistent with our hypothesis that a single integration event can kill a scid cell. An
alternative model in which active integrase molecules are released from
the infecting virion, causing damage at multiple sites with resulting scid cell death, provides a poor fit to our experimental
data (Fig. 4B). In addition, our preliminary experiments suggest that retrovirus-induced scid cell killing can be inhibited by the
reverse transcriptase inhibitor zidovudine (AZT) (unpublished results), implying that retroviral DNA, in addition to the active integrase, is
needed to induce scid cell death. Therefore, the proposal
that a single integration event is sufficient to kill a scid
pre-B cell seems to be the most plausible. This explanation is also consistent with the extreme sensitivity of such cells to DNA damage (18).
Despite this sensitivity to retrovirus-induced killing, we have shown
that some (10 to 20%) residual integration does occur in
scid cells (10), likely via an alternative,
ATM-dependent DNA repair pathway (11). In fact, the
scid lines used in our studies were derived by infection of
bone marrow cells with Abelson murine leukemia virus (A-MuLV)
(39). The report that Fulop et al. (14) were
able to isolate approximately equal numbers of v-abl
transformed colonies after infection of scid and normal bone
marrow cells with A-MuLV seems inconsistent with our observations (7). However, we note that the end point of these
experiments, cellular transformation, is quite different from the cell
viability and colony formation monitored in our experiments.
Furthermore, scid mice are known to develop lymphoid tumors
at a high frequency (9) and deficiencies in other
components of the NHEJ pathway also lead to increased tumorigenesis in
mice (12, 16, 19, 30, 37). Indeed, DNA-PKCS
has been classified as a tumor suppressor protein (23).
Thus, one possible explanation for the discrepancy with our results is
that scid bone marrow cells are more susceptible than normal
bone marrow cells to transformation by the v-abl oncogene. If so, sensitivity to retrovirus-induced killing may be obscured by
increased efficiency of transformation of the surviving infected scid cells.
How may retroviral DNA integration kill a scid cell? DNA
damage readily kills DNA repair-deficient cells (5, 15, 31, 40,
41, 43). The most lethal damage is a ds break (32, 43). According to our current understanding of the biochemistry of the retroviral integrase reaction, only the 3' ends of viral DNA are
joined to the host DNA, and single-strand gaps in the host DNA flank
the viral DNA (8, 13, 25). Host repair proteins may
respond to such gaps or other discontinuities present in the viral DNA
(8, 25). In the absence of such a response, these unrepaired regions might trigger cell death. In the integration intermediate, single-strand gaps may be in close proximity (8, 13, 25). Therefore, it is also possible that the infected cell
may "read" the integration intermediate as a ds break.
Alternatively, unrepaired gaps may become ds breaks as a result of DNA
replication. The latter explanation is consistent with our best-fitting
model's mechanism for apoptosis induction: passage through S phase and interception of a replication fork with unrepaired damage at the integration site. Lack of fit or less good fits with models that required passage through mitosis for integration is consistent with
results previously reported for ASV (22) and distinguishes this retrovirus from MuLV (36).
The assimilation of viral DNA into the host chromatin is likely to
require chromatin remodeling. As there is evidence that DNA-PK may play
a role in this process (2, 26), it is also possible that
faulty remodeling following retroviral DNA integration triggers or
contributes to scid cell death. In addition, DNA-PK activity
fluctuates during the cell cycle, with two peaks observed during
G1/early S phase and then G2 phase
(27). Thus, the differential expression or activity of
this or other critical cellular proteins in specific phases of the cell
cycle may also contribute to cell cycle effects on scid cell
killing. Repair of the integration intermediate and/or chromatin
remodeling may then be restricted to certain cell cycle phases and,
conversely, apoptosis may be initiated at these same times when the
repair does not occur.
Our results are consistent with the hypotheses that a single retroviral
DNA integration event can trigger death in cells that lack a critical
component of the NHEJ repair pathway and that the triggering event
occurs during S phase. We have recently obtained evidence that the
product of the ATM gene can respond to integration-induced damage in
such cells (11). This is in agreement with a recent report
that the ATM protein can recognize ds DNA breaks that arise during DNA
replication and direct repair machinery to such loci (24).
The basis of this extraordinary sensitivity to DNA damage and its
relevance to cellular physiology and the cell cycle can be investigated
further using retroviral genes and proteins as convenient probes.
 |
ACKNOWLEDGMENTS |
We thank T. Gales and M. Jarnik of the FCCC Electron Microscope
Facility for virus and cell measurements, R. Perry, T. London, and
Eugene Toll for critical reviews, and M. Estes for preparation of the manuscript.
This work was supported by U.S. Public Health Service grant 2P30, by
National Institutes of Health grants AI40385, CA71515, and CA06927, and
also by an appropriation from the Commonwealth of Pennsylvania.
R. Daniel and S. Litwin contributed equally to this work.
 |
FOOTNOTES |
*
Corresponding author. Mailing address: Institute for
Cancer Research, Fox Chase Cancer Center, 7701 Burholme Ave.,
Philadelphia, PA 19111. Phone: (215) 728-2490. Fax: (215) 728-2778. E-mail: AM_Skalka{at}fccc.edu.
 |
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Journal of Virology, April 2001, p. 3121-3128, Vol. 75, No. 7
0022-538X/01/$04.00+0 DOI: 10.1128/JVI.75.7.3121-3128.2001
Copyright © 2001, American Society for Microbiology. All rights reserved.
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