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Biophys J, May 1999, p. 2421-2431, Vol. 76, No. 5
RI by Multivalent Antigen
*Theoretical Biology and Biophysics, Los Alamos National Laboratory, Los Alamos, New Mexico 87545 and the Departments of #Chemistry and §Biology, Northern Arizona University, Flagstaff, Arizona 86011 USA
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ABSTRACT |
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Aggregation of cell surface receptors by multivalent
ligand can trigger a variety of cellular responses. A well-studied
receptor that responds to aggregation is the high affinity receptor for IgE (Fc
RI), which is responsible for initiating allergic reactions. To quantify antigen-induced aggregation of IgE-Fc
RI complexes, we
have developed a method based on multiparameter flow cytometry to
monitor both occupancy of surface IgE combining sites and association of antigen with the cell surface. The number of bound IgE combining sites in excess of the number of bound antigens, the number of bridges
between receptors, provides a quantitative measure of IgE-Fc
RI
aggregation. We demonstrate our method by using it to study the
equilibrium binding of a haptenated fluorescent protein, 2,4-dinitrophenol-coupled B-phycoerythrin (DNP25-PE), to
fluorescein isothiocyanate-labeled anti-DNP IgE on the surface of rat
basophilic leukemia cells. The results, which we analyze with the aid
of a mathematical model, indicate how IgE-Fc
RI aggregation depends on the total concentrations of DNP25-PE and surface IgE. As
expected, we find that maximal aggregation occurs at an optimal antigen concentration. We also find that aggregation varies qualitatively with
the total concentration of surface IgE as predicted by an earlier
theoretical analysis.
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INTRODUCTION |
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Aggregation of cell surface receptors is a common
mechanism involved in signal transduction across a cell membrane
(Metzger, 1992
). This mechanism is used, for example, by receptors that are intrinsic protein tyrosine kinases (Pazin and Williams, 1992
; Fry
et al., 1993
), such as the epidermal growth factor receptor (Schreiber
et al., 1982
) and the platelet derived growth factor receptor (Heldin
et al., 1989
), and by multichain immune recognition receptors (Keegan
and Paul, 1992
), such as the high affinity receptor for IgE (Fc
RI)
(Holowka and Baird, 1996
) and the B-cell receptor (Kaye et al., 1983
;
Kaye and Janeway, 1984
; Cambier and Ransom, 1987
). For many of these
receptors, early steps in the initiation of a signal are similar:
multivalent interactions with a ligand lead to the aggregation of
receptors and enhanced phosphorylation of tyrosines, which can be
recognized by cytoplasmic regulatory molecules. The Fc
RI receptor,
for example, is triggered when IgE-Fc
RI complexes are aggregated by
multivalent antigen. Aggregation of Fc
RI, which is constitutively
associated with the protein tyrosine kinase Lyn (Eiseman and Bolen,
1992
), then leads to a series of events, which include recruitment of
additional Lyn kinases (El-Hillal et al., 1997
; Wofsy et al., 1997
).
Signals generated by aggregation of Fc
RI, which can be negative or
positive, depend on various properties of the aggregate structures that
are formed on the cell surface. These properties include the overall
number of receptors in aggregates on the cell surface, the size of
aggregates (Fewtrell and Metzger, 1980
; MacGlashan et al., 1983
), the
spacing of receptors in aggregates (Kane et al., 1986
), and the time
that individual receptors spend in aggregates (Torigoe et al., 1998
).
For example, it has been observed that IgE dimers are less effective
than larger IgE oligomers at stimulating cellular responses (Fewtrell
and Metzger, 1980
) and that cellular responses are inhibited when an
optimal degree of aggregation is exceeded (Becker et al., 1973
; Menon
et al., 1984
; Seagrave and Oliver, 1990
). Dependency of cellular
responses on properties of receptor aggregates also has been observed
for related receptors, such as the B-cell receptor (Dintzis et al.,
1976
, 1983
) and T-cell receptor (Sloan-Lancaster et al., 1994
; Madrenas
et al., 1995
; Lyons et al., 1996
; Neumeister Kersh et al., 1998
).
Because properties of ligand-induced receptor aggregates influence the
signals that these aggregates generate, significant effort has been
devoted to quantitative analysis of interactions between multivalent
ligands and cell surface receptors, particularly in work with Fc
RI
(Goldstein, 1988
; Goldstein and Wofsy, 1994
). A goal of these studies
has been to measure or predict the number of receptors in aggregates on
the cell surface so that this quantity then can be compared and
correlated with cellular responses (Dembo et al., 1978
, 1979
; Dembo and
Goldstein, 1980
; MacGlashan and Lichtenstein, 1983
; MacGlashan et al.,
1985
). The number of receptors in aggregates is related to the number
of receptor sites in aggregates, which in turn is related to the number
of bound receptor sites in excess of the number of bound ligands. This
difference, which can be interpreted as the number of receptor pairs in
clusters (Perelson, 1981
), is zero when ligand binding is monovalent
and positive when ligand binding is multivalent because each bound ligand must engage at least one receptor site. Thus, we can quantify receptor aggregation if we can measure ligand and receptor site binding.
One method to determine both the number of ligands bound to receptors
and the occupancy of receptor sites involves differentially labeled
monovalent and multivalent ligands. This method has been used in
experiments with chemically cross-linked oligomers of IgE. For example,
by incubating rat basophilic leukemia (RBL) cells, which express
Fc
RI, with 125I-labeled dimers of IgE and then
by adding 131I-labeled IgE to assay the number of
Fc receptor sites left unbound by IgE dimers, one can determine the
number of Fc receptor sites in dimer-induced aggregates (Segal et al.,
1977
). This method works well with IgE oligomers, because IgE-Fc
RI
complexes are long lived (Kulczycki and Metzger, 1974
; Sterk and
Ishizaka, 1982
). On the time scale of an experiment, the equilibrium
between oligomeric IgE and Fc
RI is undisturbed by monomeric IgE.
However, the method is difficult to apply when receptor sites have low
affinity for sites on the multivalent ligand, as in a typical
physiological situation, because introduction of monovalent ligand can
now rapidly influence binding of the multivalent ligand to receptors.
Here, we develop a method that can be used to measure simultaneously
the amount of multivalent ligand bound to receptors and the occupancy
of receptor sites without the complication of introducing a monovalent
ligand. The method combines approaches previously used to measure the
amount of ligand bound to receptors (Seagrave et al., 1987
) and the
occupancy of receptor sites (Erickson et al., 1986
). To demonstrate the
method, we study the equilibrium binding of haptenated phycoerythrin to
anti-hapten IgE, which is labeled with fluorescein isothiocyanate
(FITC). By using two-color flow cytometry to measure fluorescence of
phycoerythrin and FITC, we are able to estimate the amount of antigen
on the surface of RBL cells and the occupancy of surface IgE combining
sites. These measurements also allow us to estimate the number of
Fc
RI pairs in antigen-induced clusters, i.e., the extent of receptor
cross-linking.
Estimates of cross-linking are refined with the aid of a mathematical
model, which we fit to data. The data are consistent with a model that
accounts for cooperative effects, which arise, at least in part, for
steric reasons. The model, which reduces to an equivalent site model
(Perelson, 1981
, 1984
; Macken and Perelson, 1985
; Lauffenburger and
Linderman, 1993
; Sulzer and Perelson, 1996
) in the absence of
cooperative effects, allows us not only to refine our estimates of
cross-linking but also to determine equilibrium binding parameters.
Furthermore, the development of this model, together with the ability
to test its predictions against experimental measurements of both
ligand binding and receptor site binding, provide new insights into
methods for quantifying multivalent ligand-receptor interactions.
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MODEL |
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To aid in analysis of experimental data, we develop a model for
equilibrium binding of 2,4-dinitrophenol-coupled B-phycoerythrin (DNP25-PE) to anti-DNP IgE-Fc
RI complexes on
RBL cells. In this model, we treat IgE-Fc
RI as a bivalent cell
surface receptor: each antibody combining site in an IgE-Fc
RI
complex represents one of two potential binding sites per receptor for
the ligand, DNP25-PE.
Reaction scheme
The model is based on the reaction scheme shown in Fig.
1 A in which ligands bind and
aggregate receptor sites through a series of reversible reactions. The
initial reaction involves the binding of solution-phase ligand to a
receptor site, and each subsequent reaction involves the addition of a
receptor site to a ligand-receptor complex (Fig. 1 B). In
this scheme, ligand-receptor complexes form without intramolecular
rearrangement reactions, i.e., without either ring or network formation
reactions (Perelson, 1984
; Macken and Perelson, 1985
). If these
reactions were significant, then the scheme in Fig. 1 A
would have to be modified.
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As indicated, the model is developed in terms of ligand states. Thus, variables in the model include the concentration of ligand in solution, which is denoted as L0, the surface density of ligand that is bound to i receptor sites, which is denoted as Li, and the surface density of free receptor sites, which is denoted as S. Related variables include the total concentration of ligand, which is denoted as LT, and the total surface density of receptor sites, which is denoted as ST.
Equilibria
To characterize the equilibria for the reactions in Fig. 1
A, we write
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(1) |
1)
characterizes the affinity of a receptor site for a ligand site when
the ligand is bound to i receptor sites (Dembo and
Goldstein, 1978
1 are identical, Eq. 1 reduces to an
equivalent site model (Perelson, 1981Cooperativity
Sites on the ligand DNP25-PE are chemically
identical: each is a DNP group. Thus, the equilibrium constants in Eq. 1 are related, although K1 through
Kn
1 need not be identical. Differences among
these equilibrium constants indicate functional nonequivalence of
ligand sites (i.e., cooperativity), which can arise for a variety of
physical reasons (Perelson, 1984
). Sites on
DNP25-PE are likely to be functionally
nonequivalent, at least in part, for steric reasons. The crystal
structure of B-phycoerythrin (Ficner et al., 1992
; Ficner and Huber,
1993
) indicates that this molecule is cylindrical with a height of 6 nm
and a diameter of 11 nm. Thus, the exposed surface area of
DNP25-PE is ~200 square nm, which is
insufficient to allow binding of more than a few DNP sites because the
area covered by a bound antibody Fab arm is at least 30 square nm
(Poljak et al., 1973
; Padlan, 1994
).
To account for functional nonequivalence of sites on
DNP25-PE, we introduce a cooperativity function
(i) to relate the cross-linking equilibrium constants
K1 through
Kn
1 (Cantor and Schimmel, 1980
):
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(2) |
(1) = 0. The functional form of
(i) is
chosen to indicate how cooperative effects are expected to influence
binding as a function of ligand site occupancy. If
(i) = 0 for all i, sites are functionally equivalent and
K1 through
Kn
1 are identical. However, for steric
reasons, we can expect the value of the cross-linking equilibrium
constant Ki to approach zero as
i approaches the effective valence of
DNP25-PE, which we expect to be much less than
the chemical valence n. This suggests that we should specify
(i) as an increasing function of i. The
simplest such form for
(i), with the required property
that
(1) = 0, is a(i
1), in which
a is a positive constant.
Conservation
Because experiments are performed under conditions that inhibit
recycling of Fc
RI, we treat the total numbers of ligands and
receptor sites as conserved quantities. Conservation of ligand can be
expressed as
|
(3) |
|
(4) |
Cross-linking
Ligand-induced aggregation of receptors is quantified by the
number of cross-links on the cell surface. A cross-link is defined as
follows (Perelson, 1981
). In the absence of intramolecular rearrangement reactions, as in the scheme of Fig. 1 A, a
ligand bound at i sites is attached to i
receptors. Thus, a ligand bound at two sites, as depicted in Fig. 1
B, forms a single cross-link, i.e., a cluster of two
receptors. If we generalize this concept of a cross-link, then a ligand
bound at i sites forms i
1 cross-links, i.e., i
1 clusters of receptor pairs. Consequently,
in the absence of intramolecular rearrangement reactions, the number of
cross-links is given by
i=1n(i
1)Li, which is equivalent to the
number of bound receptor sites
(
i=1niLi) in excess
of the number of bound ligands
(
i=1nLi).
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MATERIALS AND METHODS |
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Reagents
Mouse monoclonal anti-DNP IgE was isolated from hybridoma H1
26.82 (Liu et al., 1980
) by affinity purification (Holowka and Metzger,
1982
). Final steps in the purification process included ion exchange
chromatography to remove bound DNP-glycine, then gel filtration to
separate monomeric IgE from small amounts of IgE aggregates.
Fluorescently labeled IgE (FITC-IgE) was prepared by attaching
fluorescein-5-isothiocyanate (Molecular Probes, Eugene, OR) to IgE
(Erickson et al., 1986
). The fluorescent antigen
DNP25-PE, which is composed of 2,4-dinitrophenol
(DNP) and B-phycoerythrin (PE), was custom synthesized by Molecular
Probes. The molar ratio of DNP to PE is 25:1. The molecular weight of
DNP25-PE is ~250,000.
Cells
RBL-2H3 cells (Barsumian et al., 1981
) were grown adherent in 75 cm2 flasks. Cell cultures, which were used
typically 5 days after passage, were maintained at 37°C and 5%
CO2. Culture media consisted of MEM 1X
with Earle's salts without glutamine (Gibco BRL), 20% fetal
bovine serum (HyClone, Logan, UT), 1% v/v L-glutamine, 1% v/v penicillin, and 1% v/v streptomycin (Gibco BRL). To harvest cells,
we rinsed and then incubated the cells for 5 minutes at 37°C with
trypsin-EDTA (Gibco BRL). Cells harvested for experiments were washed
and resuspended in buffered salt solution (pH 7.7), which was freshly
passed through a 0.22-µc filter. Buffered salt solution (BSS)
consisted of 135 mM NaCl, 5 mM KCL, 1 mM MgCl2, 1.8 mM CaCl2, 5.6 mM glucose, 0.1% gelatin, and
20 mM Hepes. Cell suspensions in buffered salt solution were
supplemented with 10 mM sodium azide and 10 mM
2-deoxy-D-glucose (Sigma, St. Louis, MO) to inhibit
receptor recycling and cellular degranulation during binding
experiments. To sensitize cells to DNP, we incubated cells overnight
while cells were still in culture with excess (10 µg) anti-DNP
FITC-IgE. Sensitized cells were exposed to FITC-IgE for at least
12 h prior to harvesting.
Flow cytometric binding assays
In each binding experiment, we incubated a suspension of
sensitized cells at a density of 2.5 × 105,
106, or 4 × 106
cells/ml, with DNP25-PE at room temperature. The
concentration of DNP25-PE varied from 0.0001 to
100 µg/ml. After cells were incubated with
DNP25-PE for at least 90 min, we used a Becton Dickinson FACScan flow cytometer, which was controlled with Cell Quest
software, to collect histograms of FITC and PE fluorescence. We
determined that 90 min was sufficient for binding to reach equilibrium
at the relevant cell and ligand concentrations, because neither FITC
nor PE fluorescence varied significantly as we varied the incubation
time from 1 to 2 hours. Flow cytometric data were recorded as the mean
FITC fluorescence (520 nm) of the cell suspension, FL1, and as the mean
PE fluorescence (550 nm) of the cell suspension, FL2. To correct for
nonspecific binding of DNP25-PE to cells, we
performed a control experiment in which cells lacked surface IgE. The
difference between FL2 and the mean PE fluorescence for the control
sample,
FL2, indicates the PE fluorescence due only to specific
binding. To relate PE fluorescence to the surface density of
DNP25-PE, measurements of
FL2 were calibrated
by using microspheres embedded with a known amount of B-phycoerythrin
(Flow Cytometry Standards Corporation, San Juan, PR).
Data analysis
Relating measurements of fluorescence to binding
The fraction of surface IgE combining sites that are bound to DNP25-PE, which we denote as
, is related to
variables in the model and, as established in earlier work (Erickson et
al., 1986
|
(5) |
|
= 0), and
FL1min is FL1 when all surface IgE combining
sites are bound (
= 1). In Eq. 5, the number of bound IgE combining
sites ST
S is normalized by the total number of IgE combining sites
ST. Below, we also use
ST to normalize quantities that
characterize DNP25-PE binding and cross-linking,
because neither the number of bound DNP25-PE molecules nor the number of cross-links can be greater than the total
number of IgE combining sites.
The ratio of cell-bound DNP25-PE to surface IgE
combining sites, which we denote as
, is related to variables in the
model and, as established in earlier work (Seagrave et al., 1987
|
(6) |
FL2 is PE fluorescence due to specific binding of
DNP25-PE to surface IgE and
FL2max is
FL2 when
DNP25-PE binding is saturated, i.e., when each
IgE combining site is bound to one molecule of
DNP25-PE (
= 1).
Based on our earlier definition of a cross-link, the number of
cross-links per IgE combining site, which we denote as
, is related
to
and
as follows:
|
(7) |
indicates the normalized number of clustered IgE-Fc
RI pairs. In the
presence of these reactions,
is still related to cross-linking; however, in this case,
is no longer directly proportional to the
number of cross-links.
Estimating parameters by fitting the model to data
Three sets of data were used to determine best-fit values for K0, K1, ST, and a, where a is a parameter in the specified cooperativity function
(i). We considered various one-parameter functional forms
for
(i), including
(i) = a(i
1). Each data set consisted of
measurements of FITC fluorescence (FL1) and PE fluorescence (
FL2)
for a series of ligand concentrations. These measurements were taken at
one of three cell densities: 2.5 × 105,
106, or 4 × 106
cells/ml. Because data sets were collected with different instrument settings, it was necessary to determine best-fit scaling factors (FL1min, FL1max, and
FL2max) for each set of FL1 and
FL2 measurements.
Best-fit parameter values were determined by using the FORTRAN
subroutine DNLS1 from the SLATEC Common Mathematical Library (http://www.netlib.org/slatec), which implements a modified
Levenberg-Marquardt algorithm for solving nonlinear least-squares problems.
Solving the model equations
Equilibrium states are calculated by solving the model equations, which is aided by combining Eqs. 1-4. By using Eq. 1 to express each Li as a function of S and L0, by using Eq. 2 to relate K1 through Kn
1, and by using Eq. 3 to express
L0 as a function of S, we
can rewrite Eq. 4 to obtain
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(8) |
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(9) |
(0) = 0. Cooperative
effects are included entirely in the exponential term of Eq. 9. If this
term reduces to 1, Eqs. 8 and 9 reduce to an equivalent site model.
When values for the parameters (n, C,
LT,
ST,
K0, and
K1) and a functional form for the
cooperativity function
(i) are specified, Eq. 8 is a
nonlinear equation involving a single unknown: the fraction of free
receptor sites S/ST. To
determine the fraction of free receptor sites at equilibrium, we solve
this equation by using the method of bisection (Press et al., 1992
i=1n
(i)]
and
Li/ST = (K0LT)(L0/LT)
(i),
which are derived from Eqs. 1-3.
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RESULTS |
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We use multiparameter flow cytometry to study the equilibrium
binding of a multivalent ligand to a cell surface receptor. The ligand,
DNP25-PE, is haptenated phycoerythrin (PE): each
molecule of PE is coupled to an average of 25 DNP molecules. The
receptor for this ligand is FITC-labeled anti-DNP IgE that is bound to Fc
RI on the surface of RBL cells. Below, we first present
qualitative features of DNP25-PE binding to
surface IgE, and we then illustrate how measurements of PE and FITC
fluorescence can be used to quantify antigen-induced aggregation of
IgE-Fc
RI complexes. The methods developed here allow us to determine
how equilibrium cross-linking varies quantitatively with the total
concentrations of ligand and receptor.
Qualitative features of antigen binding to surface IgE
In our experiments, DNP25-PE at various
concentrations is added to suspensions of RBL cells that have been
sensitized with FITC-IgE. Then, after equilibrium is reached, PE and
FITC fluorescence are measured simultaneously in a flow cytometer.
Fluorescence measurements for a series of experiments are shown in Fig.
2. As the concentration of
DNP25-PE increases, FITC fluorescence (FL1)
decreases and PE fluorescence (
FL2) increases. A decrease in FITC
fluorescence indicates an increase in the occupancy of IgE combining
sites (Erickson et al., 1986
), and an increase in PE fluorescence
indicates an increase in association of DNP25-PE with the cell surface (Seagrave et al., 1987
).
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Receptor binding saturates before ligand binding
As can be seen in Fig. 2, receptor sites saturate (i.e., FL1 reaches a lower plateau) at a ligand concentration of ~0.1 µg/ml, whereas ligand binding, as measured by
FL2, fails to reach an obvious plateau even at ligand concentrations greater than 10 µg/ml.
This effect cannot be explained by nonspecific binding of ligand to
cells, which was assayed in control experiments, because
FL2
represents the PE fluorescence due only to specific binding. We expect
that
FL2 continues to rise after FL1 reaches a plateau for the
following reason. When FL1 first reaches a plateau, ligand binding is
multivalent. Then, as the ligand concentration increases, the
multiplicity of ligand binding decreases, which allows more ligand to
bind to the cell surface. As a result,
FL2 increases. This
explanation is consistent with the binding parameters that we later determine.
Ligand binding approaches saturation
At ligand concentrations greater than 20 µg/ml, measurements of PE fluorescence are unreliable due to light scatter. Thus, we are unable to measure PE fluorescence at saturation (i.e., we are unable to measure
FL2max) as is required to directly
relate measurements of PE fluorescence to the extent of ligand binding (Eq. 6). Nevertheless, by using microspheres embedded with a known amount of PE to calibrate measurements of
FL2, we are able to estimate the extent of ligand binding. The calibration results indicate
that the highest recorded value of
FL2 in Fig. 2 (1380) corresponds
to ~9 × 105 PE molecules per cell and at
least the same number of receptor sites per cell (each bound ligand
engages at least one receptor site). Thus, ligand binding approaches
saturation in the experiments of Fig. 2 because RBL cells only express
300,000 to 600,000 Fc
RI receptors per cell (Erickson et al., 1987
RI receptors per cell, we can
estimate that the highest recorded value of
FL2 is within at least
75% of
FL2max because the minimum number of
receptor sites per cell indicated by bead calibration (9 × 105) is 75% of the maximum number of surface IgE
combining sites per RBL cell (1.2 × 106).
As we will see later, model-based analysis indicates that ligand binding actually approaches 90% saturation in the experiments of Fig.
2.
Quantifying antigen-induced aggregation of surface IgE sites
We quantify receptor aggregation by determining the number of
bound receptor sites in excess of the number of bound ligands. To
determine this quantity, which we interpret as the number of cross-links, we must measure or estimate the scaling factors in Eqs.
5-7 (FL1min, FL1max, and
FL2max) and then use these equations to relate
measurements of fluorescence (FL1 and
FL2) to quantities that
characterize ligand and receptor binding (
,
, and
).
Fluorescence measurements directly indicate a lower bound on cross-linking
The highest recorded value of
FL2 represents a lower bound on
FL2max. By using this lower bound, we can
place an upper bound on the extent of ligand binding and a lower bound
on the extent of cross-linking, as can be seen by inspecting Eqs. 6 and
7. In Eq. 6, the number of bound ligands per receptor site
is
defined as
FL2/
FL2max. Thus, an
underestimate of
FL2max leads to an overestimate of
. In Eq. 7, the number of cross-links per receptor site
is defined as
. Thus, an overestimate of
leads
to an underestimate of
.
In Fig. 3, we show how the fluorescence
measurements of Fig. 2 are related to biologically meaningful
quantities. In Fig. 3 A, we plot receptor site occupancy
, which is calculated by using Eq. 5, as a function of ligand
concentration. The scaling factors FL1min and
FL1max, which appear in Eq. 5, are readily determined from the fluorescence data (Fig. 2). In Fig. 3 B,
we plot the extent of ligand binding
, which is calculated by using Eq. 6, as a function of ligand concentration. The values of
were
calculated by using the highest recorded value of
FL2 for
FL2max in Eq. 6. Because we have determined
only that this value is within 75% of
FL2max
(on the basis of our bead calibration results), values of
are
uncertain to the extent indicated by the error bars. However, as
illustrated, the fluorescence data directly indicate an upper bound on
ligand binding. In Fig. 3 C, we plot the extent of
cross-linking
, which is calculated by using Eq. 7, as a function of
ligand concentration. As illustrated, an upper bound on
translates
to a lower bound on
. Note that the increasing portion of the
cross-linking curve is insensitive to the estimated uncertainty in
FL2max.
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Model-based analysis of fluorescence data yields refined estimates of receptor site occupancy, ligand binding, and cross-linking
To aid in the analysis of fluorescence data, we developed a model for ligand-receptor binding (Eqs. 1-4). We simultaneously fit this model to three data sets, one of which is that shown in Fig. 2. Each data set was collected at a different cell density. The following best-fit parameter values, which apply for all three data sets, were determined: K0 = 4.4 × 108 M
1,
K1ST = 13, and
ST = 9.6 × 105 sites/cell. The fitting procedure also
allowed us to specify a = 0.43 for the cooperativity
function
(i) = a(i
1). We
considered a variety of one-parameter functional forms for
(i), but functions consistent with the data indicated
essentially the same values for the cross-linking equilibrium constants
K1 through
Kn
1. In addition to these parameter values, we
also determined for each data set best-fit values for the scaling
factors FL1min, FL1max, and
FL2max. For example, we determined that
FL2max = 1500 for the data set of Fig. 2,
which indicates that ligand binding in these experiments reached
~90% saturation (1380/1500).
The extent to which the model fits the data is illustrated in Fig.
4. Both the fraction of bound receptor
sites and the number of bound ligands per receptor site are plotted as
a function of ligand concentration. The points are derived from the
fluorescence data of Fig. 2, Eqs. 5 and 6, and the best-fit scaling
factors. These plots meet two expectations. First, the fraction of
bound receptor sites
is greater than or equal to the number of
bound ligands per receptor site
. This result is expected because
each bound ligand must engage at least one receptor site. Thus,
must be greater than
when ligand binding is multivalent, and
must equal
when ligand binding is monovalent. Second,
and
converge at high ligand concentrations, which indicates that ligand
binding is predominantly monovalent at these concentrations. The
quality of the fit illustrated in Fig. 4 is typical of the fits for the other two data sets.
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RI receptors (300,000 to 600,000 per
cell) that are expressed on RBL cells (Erickson et al., 1987
1, is comparable
with the affinity of anti-DNP IgE for DNP on haptenated bovine serum
albumin, 8.5 × 108
M
1 (Xu et al., 1998
(i) = 0.43(i
1) is an increasing function of ligand site
occupancy i. Also, as is consistent with the structures of Fab and PE, theoretical values for the ratio
/
, which indicates the number of bound receptor sites per bound ligand molecule, are much
less than the chemical valence of DNP25-PE. For
example,
/
4 at 0.1 µg/ml in Fig. 4 is where the
cross-linking curve peaks (Fig. 5).
Cross-linking is indicated by the vertical distance between the two
curves in Fig. 4 because
=
(Eq. 7).
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Dependence of cross-linking on ligand and receptor concentration
In Fig. 5, we plot the extent of cross-linking
as a function
of ligand concentration for three cell densities. The points are
derived from fluorescence measurements by using Eqs. 5-7 and best-fit
scaling factors. Each curve indicates how cross-linking varies as a
function of ligand concentration at a particular cell density or
equivalently a particular receptor or receptor site concentration. Each
of these cross-linking curves is bell shaped, as expected.
Cross-linking increases with ligand concentration up to an optimal
ligand concentration and then decreases as monovalent binding, because
of excess ligand, begins to predominate.
The results shown in Fig. 5 indicate that cross-linking is influenced
by the cell density. Three features are discernible. First, the
location of the increasing portion of the cross-linking curve depends
on the cell density. This portion of the curve, which corresponds to
the regime where receptor sites are not saturated, shifts to the right
as the cell density increases. Thus, at a fixed ligand concentration,
cross-linking decreases as the cell density increases if receptor site
binding is below saturation. Second, the peak of the cross-linking
curve is independent of cell density, i.e., each curve has the same
maximum height. Third, the location of the decreasing portion of the
cross-linking curve, which corresponds to the regime where receptor
sites are saturated, tends not to depend on the cell density. As can be
seen, the three curves coincide at ligand concentrations greater than 1 µg/ml. These qualitative features of cross-linking curves were
predicted in an earlier theoretical analysis (Sulzer and Perelson,
1996| |
DISCUSSION |
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|
|
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In many antigen, hormone, and cytokine receptor systems, signal
transduction is initiated by aggregation of cell surface receptors (Metzger, 1992
). However, even in the well-studied Fc
RI system, the
features of ligand-receptor binding that are critical for signaling
have yet to be fully characterized, especially for cases in which the
ligand has more than two binding sites. Here, we have developed and
applied a flow cytometric method to monitor receptor site occupancy
(Figs. 3 A and 4), ligand binding (Figs. 3 B and
4), and cross-linking (Figs. 3 C and 5). This study, like the recent work of Xu et al. (1998)
, represents an attempt to quantify
the interactions of a multivalent antigen with IgE-Fc
RI.
The method that we have developed to quantify Fc
RI aggregation is
significant for several reasons. First, the antigen is a haptenated
protein (DNP25-PE) that resembles a physiological allergen. Like an allergen, it elicits strong cellular responses (Seagrave et al., 1987
). This is in contrast to bivalent haptens (Siraganian et al., 1975
; Kane et al., 1986
; Posner et al., 1995a
). Also like an allergen, DNP25-PE cross-links
Fc
RI via antigen-antibody reactions. This is in contrast to
oligomers of IgE; the kinetics of IgE binding to Fc
RI differ
significantly from typical antigen-antibody kinetics (Kulczycki and
Metzger, 1974
; Sterk and Ishizaka, 1982
). Second, the method allows us
to characterize reactions on the cell surface without disturbing these
reactions. This is in contrast to another flow cytometric method that
recently has been developed to study multivalent ligand-receptor
binding (Woodard et al., 1995
). In this method, which we discuss later,
a labeled monovalent ligand is used to determine the number of receptor
sites that are bound by a differentially labeled multivalent ligand.
Third, our method can be applied not only in equilibrium binding
studies, as we have demonstrated here, but also in kinetic studies
(Posner et al., 1998
). Kinetic binding studies may be important for
understanding the temporal properties of Fc
RI aggregates that
influence signaling (MacGlashan et al., 1985
; Torigoe et al., 1998
).
We quantify receptor aggregation by determining two quantities: the
number of bound receptor sites and the number of bound ligands. These
quantities reveal information about the state of receptor aggregation.
For example, if the number of bound ligands equals the number of bound
receptor sites, then each ligand is bound to a single receptor site and
no receptors are aggregated. In the absence of intramolecular
rearrangement reactions, the number of bound receptor sites in excess
of the number of bound ligands can be interpreted as the number of
cross-links, i.e., the number of clustered receptor pairs (Perelson,
1981
). We assume that this interpretation is valid here, i.e., we say
that a cross-link is formed each time two receptor sites are joined.
However, our use of this assumption does not represent a limitation of
the method because cross-linking can be determined more directly if bispecific chimeric IgE is available. In experiments with this reagent,
receptor aggregation is equivalent to receptor site aggregation, which
is indicated by the number of bound receptor sites in excess of the
number of bound ligands.
One approach that has been used to quantify Fc
RI aggregation
involves oligomers of IgE (Segal et al., 1977
). The number of bound
oligomers is determined by radiolabeling. Monomeric IgE labeled with a
different isotope is then used to determine the number of free Fc
RI
receptors. Because dissociation of IgE from Fc
RI is slow (Kulczycki
and Metzger, 1974
; Sterk and Ishizaka, 1982
), it is possible to add
oligomeric IgE, reach equilibrium, and then add excess monomeric IgE to
fill empty Fc sites without disturbing oligomer binding on the time
scale of the experiment. Although oligomers of IgE are useful tools for
studying receptor aggregation and subsequent cellular responses in this
system, they have a number of limitations (Goldstein, 1988
). Aggregates can be no larger than the number of chemically cross-linked IgE molecules, so IgE oligomers are unable to produce signals that depend
on large receptor aggregates. Binding of IgE to Fc
RI is slow, so it
may be difficult to separate the kinetics of oligomer binding from the
kinetics of the cellular response. Also, IgE oligomers produce
long-lived cross-links, and thus their effects may be atypical because
signaling events that require the continual formation of new
cross-links will not be observed.
Recently, Woodard et al. (1995)
used a multivalent antigen to aggregate
B-cell receptors and then used a differentially labeled monovalent
antigen to count free receptor sites. Two-color flow cytometry was used
together with FITC-DNP-L-papain, as a monovalent antigen,
and TRITC-DNP-pol or TRITC-DNP-dextran, as a multivalent antigen, to
determine the amount of monovalent antigen and the amount of
multivalent antigen bound to DNP-specific B cells. Data obtained with
this indirect method are difficult to interpret because the reactions
are reversible (the typical dissociation rate constant for a bond
between DNP and an antibody combining site is between 0.1 and 0.001 s
1). Thus, on the time scale of these
experiments, the binding of multivalent antigen is disturbed when the
monovalent antigen is added to the system. In comparison, our method of
measurement does not require an additional monovalent probe. Thus, it
avoids the complications that arise when different ligands compete for the same receptor. However, our approach requires that we label the
receptors, which is impossible if the receptor is unavailable in a
secreted form or cannot be reattached to the cell surface. The second
condition is not fulfilled for many receptors, and consequently, an
indirect method such as that used by Woodard et al. (1995)
is then
required to measure aggregation.
Another approach used to study Fc
RI aggregation involves symmetric
bivalent ligands, which represent the simplest type of ligand capable
of aggregating receptors. Mathematical models have been developed for
bivalent ligands interacting with bivalent cell surface receptors
(Dembo and Goldstein, 1978
; Perelson and DeLisi, 1980
; Perelson, 1980
;
Wofsy and Goldstein, 1987
; Posner et al., 1995b
). However, a major
limitation of these ligands is their inability to activate strong
cellular responses. A variety of evidence suggests that these ligands
are poor activators of cellular responses because they aggregate
receptors predominantly in the form of stable cyclic dimers (Kane et
al., 1986
; Schweitzer-Stenner et al., 1987
; Erickson et al., 1991
;
Posner et al., 1991
; Posner et al., 1995a
). Cyclic dimers, in which two
ligand molecules connect two IgE-Fc
RI complexes to form a closed
ring, prevent chain elongation and limit the size of ligand-induced
aggregates. With ligands of larger valence, such as
DNP25-PE, ring formation does not necessarily prevent growth of receptor aggregates. Thus, multivalent ligands are
capable of cross-linking many IgE molecules and typically initiate
strong cellular responses. When interacting with surface IgE, these
ligands can form chain-, ring-, tree-, and network-like structures,
whereas bivalent ligands can form only chain- and ring-like structures.
This advantage of multivalent ligands is also a disadvantage, because a
theory that describes the binding of multivalent ligands to bivalent
receptors has yet to be fully developed. However, in a variety of
related reaction systems studied in polymer chemistry, it has been
found that ignoring the intramolecular reactions that form rings and
networks leads to results that adequately characterize most aggregates
(Flory, 1953
), except those that form rubber-like materials. For these
reasons, we have used a theory of multivalent ligand-receptor
interactions that accounts for chain- and tree-like but not ring- and
network-like aggregate structures. The model based on this theory is
consistent with our binding data (Figs. 4 and 5).
In our efforts to estimate parameter values, we observed that unique
best-fit parameter values are difficult to determine. To address this
problem, we used three independent data sets, each collected at a
different cell density and each consisting of both FL1 and
FL2
measurements. We obtain different results if we fit only FL1 data, only
FL2 data, or only data at a single cell density (unpublished
material). This suggests that models of multivalent ligand-receptor
interactions should be tested with a global analysis of multiple data
sets (Posner and Dembo 1994
; Myszka et al., 1998
).
In summary, we have demonstrated a method by which the number of
cross-links can be determined when both the number of receptor sites
occupied and the number of ligands bound per receptor site are measured
simultaneously. With this technique, we have confirmed that the
equilibrium cross-linking curve is bell shaped (Figs. 3 C
and 5). The results shown in Fig. 5 also confirm qualitative predictions concerning the influence of cell density on the
cross-linking curve (Sulzer and Perelson, 1996
). As predicted, we
observe that an increase in cell density shifts the increasing portion
of the cross-linking curve toward higher ligand concentrations, that the maximum height of the cross-linking curve is independent of cell
density, and that the decreasing portion of the cross-linking curve
also is independent of cell density. Thus, the equivalent site model
studied by Sulzer and Perelson (1996)
apparently can be used to predict
the qualitative features of cross-linking curves for real ligands.
However, to obtain quantitative estimates of binding parameters and
more accurate quantification of ligand-receptor aggregation, it was
important here to consider a more complicated model that included
negative cooperativity due to steric effects. In conclusion, we have
developed new theoretical and experimental tools for studying
multivalent ligand-receptor binding.
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ACKNOWLEDGMENTS |
|---|
We thank B. Goldstein for helpful discussions.
This work was performed under the auspices of the U.S. Department of Energy and was supported by Grants RR06555 and AI28433 to ASP and by Grant AI35997 to RGP from the National Institutes of Health.
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FOOTNOTES |
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Received for publication 9 December 1997 and in final form 11 January 1999.
Address reprint requests to Dr. Alan S. Perelson, T-10, MS K710, Los Alamos National Laboratory, Los Alamos, NM 87545. Tel.: 505-667-6829; Fax: 505-665-3493; E-mail: asp{at}lanl.gov.
Reprint requests may also be addressed to Dr. Richard G. Posner, Department of Chemistry, Northern Arizona University, Flagstaff, AZ 86011. Tel.: 520-523-4209; Fax: 520-523-8111; E-mail: richard.posner{at}nau.edu.
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