Endocrinology Vol. 138, No. 4 1456-1463
Copyright © 1997 by The Endocrine Society
Differential Sensitivity of Thyroid Hormone Receptor Isoform Homodimers and Mutant Heterodimers to Hormone-Induced Dissociation from Deoxyribonucleic Acid: Its Role in Dominant Negative Action
Xu-Guang Zhu,
Peter McPhie and
Sheue-yann Cheng
Laboratory of Molecular Biology (X.-G.Z., S.-y.C.), Division of
Basic Sciences, National Cancer Institute, and Laboratory of
Biochemical Pharmacology (P.M.), National Institute of Diabetes,
Digestive and Kidney Diseases, NIH, Bethesda, Maryland 20892-4255
Address all correspondence and requests for reprints to: Dr. Sheue-yann Cheng, Building 37, Room 2D24, 37 Convent Drive MSC 4255, Bethesda, Maryland 20892-4255. E-mail: sycheng{at}helix.nih.gov
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Abstract
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General resistance to thyroid hormone is an inheritable disease with
resistance of peripheral tissues to elevated levels of thyroid hormone.
Genetic studies have shown that it is due to interference in the
functions of wild-type thyroid hormone nuclear receptors (wTRs) via the
dominant negative effect of mutant TRs (mTRs). The present study
compared the heterodimerization of the two TR isoforms, TRß1 and
TR
1, with mutant TRs to understand if mTRs had isoform-dependent
dominant negative action. Using electrophoresis gel mobility shift
assay, we have demonstrated that mutant PV, S, ED, and OK form
heterodimers with wTR
1 and
TRß1 (in which the A/B domain of
wTRß1 has been deleted), on the F2-thyroid hormone response element
(TRE). In the presence of T3, both homo- and heterodimer
complexes are dissociated in a T3 concentration dependent
manner. The ED50 for
TRß1 homodimers was 3-fold higher
than that of wTR
1 homodimers. ED50s for
TRß1/mTR
heterodimers were 10- to 40-fold higher than the corresponding
wTR
1/mTR heterodimers. Mutant ED and OK homodimers were only
partially dissociated at the highest T3 concentrations used
(100 nM), whereas no dissociation could be detected for PV
and S homodimers, indicating differential sensitivity of the F2-bound
TR dimers to the T3-induced dissociation. We presented a
model that indicates the dissociation of any particular TR dimer from
F2 is determined by competition of T3 for both of its
constituent TRs. By transfection assays, we showed that the potency of
the dominant negative action of PV on TR
1 and TRß1 inversely
correlated with the sensitivity of the appropriate mTR/wTR heterodimer
to T3-induced dissociation from F2. The differential
dominant negative action of mutants on the two TR isoforms could play
an important role in the heterogeneity of tissue-specific
manifestations in patients with resistance to thyroid hormone.
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Introduction
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RESISTANCE TO thyroid hormone (RTH) is an
inheritable disorder characterized by an inappropriately normal or
elevated level of TSH accompanied by resistance of the pituitary and
peripheral tissues to the action of elevated circulating levels of
thyroid hormones (1, 2). These may accompanied by one or several
phenotypic features with variable degrees of tissue resistance to
thyroid hormones (1, 2, 3). Classical features include goiter, decreased
IQ, dyslexia, tachycardia, delayed bone maturation, attention-deficit
hyperactivity disorder, and short stature. There is considerable
heterogeneity in the degree of severity and the affected organs among
individuals and kindreds with RTH (1, 2).
Genetic analyses of the affected kindreds indicate that the clinical
manifestations of RTH patients are due to the interference of the
functions of the wild-type thyroid hormone nuclear receptors (wTRs) via
the dominant negative effect of the mutant TRs (mTRs). wTRs are
ligand-dependent transcription factors that are the products of two
genes,
and ß. Each gene gives rise to two subtypes,
1,
2,
ß1, and ß2, by alternative splicing of the primary transcripts.
wTRs regulate the functions of thyroid hormone target genes by binding
to the specific DNA sequences known as the thyroid hormone response
elements (TREs). Four domains can be assigned to each TR, domains A/B,
C, D, and E. Domain C contains two zinc fingers and is involved in
binding of the receptors to TREs. Domains D and E are structurally
linked, in so far as part of domain D is required for the biological
function of domain E, which is to bind to the thyroid hormone,
T3 (4, 5). Domains D and E are also involved in binding to
corepressors and dimerization, respectively (6, 7). Except for one
recent report in which a naturally occurring mutation in TR
gene was
detected in a human hepatocarcinoma cell line derived from a patient
(8), the mutations detected so far in RTH patients only occur in the
TRß gene. Most of the mutations are missense mutations that are
clustered in two hot spots: one is in the middle of the T3
binding domain, and the other is close to the C-terminus. The
functional impairments of mTRß1 include variably reduced or absent
T3 binding, reduced or absent transactivation capacity, and
dominant negative potency (1, 2, 9, 10).
Three nonmutually exclusive mechanisms have been proposed to account
for the dominant negative action of mTRß1: 1) competition of wTRs and
mTRß1 for binding to TREs; 2) competition by wild-type and mutant
receptors for limiting amounts of TR-associated proteins or other
nuclear factors essential for transcription (11, 12); 3) formation of
inactive wild-type/mutant heterodimers that may limit access by
transcriptionally relevant TR complexes to DNA and thus contribute to
the dominant negative effect of mutant receptors. To date, this third
mechanism has been the least studied, probably due to the difficulty of
a convincing demonstration of the formation of wild-type/mutant
receptor heterodimers. Recently, however, we have circumvented this
problem by using a truncated form of TRß1 (
TRß1) in which the
A/B domain was deleted. Deletion of A/B domain has no effect on the
binding of wTRß1 to T3 and TREs (13). Using mutant PV
that has a frame-shift mutation in the last 16 amino acids, we
showed clearly the formation of wTRß1/PV heterodimers by
electrophoretic mobility gel shift assay (EMSA). Furthermore, we showed
that there is a strong correlation between the formation of wTRß1/PV
heterodimers and the dominant negative potency of PV (13).
However, it is still unknown whether wTRß1 also forms heterodimers
with other mutants. More importantly, at present, the role of
wTR
1/mTR heterodimers in the dominant negative effect of mutants is
unknown because formation of wTR
1/mTR heterodimers has not yet been
demonstrated. We therefore examined the interaction of four mutants
with wTRß1 and wTR
1 on F2-TRE in which the half-site binding
motifs are arranged in an everted-repeat. We found that both isoforms
form heterodimers with four mutants on F2. Furthermore, the sensitivity
of the F2-bound heterodimers to T3-induced dissociation was
mutant- and isoform-dependent.
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Materials and Methods
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Cell culture media were purchased from BioWhittaker
(Walkersville, MD). FCS and lipofectamine transfection reagent were
obtained from GIBCO-BRL (Grand Island, NY).
5'-[
-32P]-dCTP (6000 Ci/mmol) was obtained from
Amersham Life Science (Arlington Heights, IL).
[14C]-Chloramphenicol and
3'-[125I]-T3 were purchased from DuPont New
England Nuclear (Boston, MA). TNT-coupled reticulocyte lysate in
vitro translation kits were from Promega (Madison, WI).
Plasmids
The T7 expression plasmid pJL08 encoding a truncated wTRß1 in
which the A/B domain (amino acids 1105) was deleted has been
described previously (5). The T7 expression plasmids pCLC13 and pCJ3
encoding wTR
1 and wTRß1, respectively, were prepared as described
(14, 15). The reporter plasmids, pF2-thymidine kinase
promoter-chloramphenicol acetyltransferase (pF2-TK-CAT) was a gift
from Dr. G. Brent. The plasmids pGEM3Z-PV, pGEM3Z-S, pGEM3Z-OK,
pGEM3Z-ED encoding mutant PV, S, OK and ED, respectively, were gifts
from Dr. C. A. Meier.
Transfection assay
CV1 cells were plated 24 h before transfection in DMEM
containing 10% T3-depleted FCS in 60-mm Petri dishes at a
density of 4 x 105 cells/dish. The cells were
transfected by the appropriate plasmids using lipofectamine according
to the manufacturers instructions. After 24 h, the medium was
replaced with fresh DMEM containing 100 nM of
T3. After incubation for an additional 24 h, cells
were harvested and lysed. The transfection efficiency was monitored by
ß-galactosidase activities, and the CAT activity was normalized to
the protein concentration of the lysates.
Electrophoresis gel mobility assay (EMSA)
Two complementary oligonucleotides containing F2 sequences
(shown below) were annealed and the recess 3'-end filled with DNA
polymerase (Klenow fragment) in the presence of
[
-32P]-dCTP.
The labeled oligonucleotides were separated on a 12%
polyacrylamide gel and purified by electroelution. The gel mobility
shift assay was carried out as below: in vitro translated TR
receptor proteins were incubated with the labeled oligonucleotides in
the binding buffer (25 mM HEPES, pH 7.5, 5 mM
MgCl2, 4 mM EDTA, 10 mM DTT, 0.11
M NaCl and 0.4 µg single-stranded DNA). After incubation
for 30 min at 25 C, the reaction mixture was loaded onto a 5%
polyacrylamide gel and electrophoresed at 4 C for 23 h at a constant
voltage of 250 V. The gel was dried and autoradiographed. The
intensities of the retarded bands and free oligonucleotides were also
quantified by PhosphoImager (Molecular Dynamics, CA). The binding data
were analyzed based on the equations and methods described by Zhu
et al. (13).
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Results
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Both wTRß1 and wTR
1 can form heterodimers with mutants
We have recently shown that wTRß1 forms heterodimer with mutant
PV on TREs (13). Among the three TREs in which the half-site binding
motifs arranged in three different orientations, wTRß1 binds to F2
with highest affinity as a homodimer and as a heterodimer with mutant
PV (13). PV has a frame-shift mutation in the last 16 amino acids of
TRß1 and has virtually lost its T3 binding activity (10;
Table 1
). Because it is not known whether the formation
of heterodimers between the TRß1 and mutant is only limited to PV or
it is a more general phenomenon, we evaluated whether other mutants
also form heterodimers with TRß1. We chose three other mutants as
representatives (Table 1
). Mutants S and ED (A317T) are located in the
first hot spot. Mutant S has a codon deletion on 337 (
337) and like
mutant PV, has completely lost T3 binding activity (10).
Mutant OK (M442V), like PV, is located in the second hot spot. Both
mutants, OK and ED, have a missense mutation, resulting in a reduction
of 78% of T3 binding activity. Therefore, these four are
representatives of mutants in terms of the location of hot spots and
T3 binding affinity.
Previously, to clearly demonstrate the formation of heterodimers by
EMSA, it was necessary to use
TRß1 in which the A/B domain of
wTRß1 has been deleted. Deletion of A/B domain has no effect on the
T3 and DNA binding activity (13). Therefore, we used
TRß1 to demonstrate the formation of heterodimers of TRß1 with
other mutants. Figure 1A
shows that in the presence of
equal amounts of mutant S and
TRß1 proteins, three well-resolved
bands, representing F2-bound S/S, S/
TRß1 and
TRß1/
TRß1
dimers in an approximate ratios of 1:2:1, were seen (lanes 16). These
results are similar to those seen for PV (13). Lanes 7 and 8 of Fig. 1A
show the positions of
TRß1/
TRß1 and S/S homodimers,
respectively. The intensities of these three bands increased in a
F2-concentration dependent manner (lanes 16 of Fig. 1A
). We
determined the apparent affinity constants (Ka) in the
binding of S/S, S/
TRß1 and
TRß1/
TRß1 dimers to F2. As
shown in Table 2
, these three dimers bound to F2 with
very similar apparent binding affinity constants, indicating that the
deletion of codon 337 (see Table 1
) had no effect on the formation of
S/S homodimers and S/
TRß1 heterodimers. We further carried out
similar binding experiments for mutant ED (Fig. 1B
) and mutant OK (Fig. 1C
). Again, formation of three well separated mutant/mutant,
mutant/
TRß1 and
TRß1/
TRß1 bands in a F2-concentration
dependent manner was seen (lanes 16 of Fig. 1
, B and C). We also
determined their Ka to F2. As shown in Table 2
, within
experimental errors, there were no significant differences in
Ka not only for binding to F2 for different dimers, but
also for different mutants. The Ka for the binding of
PV/PV, PV/
TRß1 and
TRß1/
TRß1 to F2 that were determined
previously were also included in Table 2
for comparison (13). These
results indicate that in the absence of T3, the dimeric
binding of mutant/mutant and mutant/
TRß1 to F2 was independent of
mutation sites for these four mutants.
We further examined whether wTR
1 forms heterodimers with mutants.
Lanes 9 and 8 of Fig. 2
, A and B, respectively, show
that different from the binding of
TRß1 to F2 (lane 7 of Fig. 1A
),
wTR
1 bound to F2 both as a homodimer and monomer (13, 16, 17). Lanes
8 and 9 of Fig. 2
, A and B, show the binding of S and PV, respectively,
as a homodimer to F2. In the presence of equal amounts of either mutant
S (lanes 17 of Fig. 2A
) or mutant PV (lanes 17 of Fig. 2B
), in
addition to the wTR
1 monomer, three discrete dimeric bands,
representing mutant/mutant, mutant/wTR
1, and wTR
1/wTR
1 were
seen, indicating that, similar to
TRß1, wTR
1 can also form
heterodimers with mutants. As shown in Fig. 2
, the binding of wTR
1
as monomer and three dimers to F2 was F2 concentration dependent.
However, because of the complexity in the analysis of simultaneous
multiple equilibria of the four binding species (three dimers and one
monomer), we were unable to set up equations to determine
accurately the Ka for each binding species. However,
experiments shown in Fig. 2
, A and B, were carried out under the
same experimental conditions and the intensities of homodimeric and
heterodimeric bands quantified by PhosphoImager were identical for
mutant S and PV at each F2 concentration (e.g. the
intensities of homodimeric and heterodimeric bands in lanes 7 of Fig. 2
, A and B). Based on the identical intensities of the dimeric and
monomeric bands, it is reasonable to conclude that there was no
significant differences in the Ka between the binding
of S/S and PV/PV, of S/wTR
1 and PV/wTR
1 dimers to F2. We also
carried out the binding experiments for ED and OK similarly. We found
that the intensities of F2-bound ED/ED and OK/OK homodimeric bands and
F2-bound ED/wTR
1 and OK/wTR
1 heterodimeric bands, at each F2
concentration (data not shown), were similar to those of S/S and
S/wTR
1, respectively. These results indicate that both TR isoforms
could form heterodimers with many mutant TRs and that the binding of
mutant/wild-type TR heterodimers to F2 is independent of the mutation
sites in the four mutants examined.
Differential sensitivity of F2-bound homodimer and heterodimer of
TR isoforms to the T3-induced dissociation
In the presence of T3, however, a dramatically
different picture emerged in the binding of homodimers and heterodimers
of TR isoforms to F2. Figures 3D
and 4I
-A
show that wTRß1/wTRß1,
TRß1/
TRß1 and wTRß1/
TRß1
dimers were similarly dissociated by T3 in a
concentration-dependent manner, indicating that domain A/B has no
effect on the T3-induced dissocation of TRß1 homodimers.
Figure 3A
shows that while
TRß1/
TRß1 was dissociated by
increasing concentrations of T3, S/
TRß1 and S/S dimers
were not affected by T3 up to 100 nM. These
findings were similar to that found for PV/
TRß1 and PV/PV dimers
(13). However, not all mutant/
TRß1 heterodimers and mutant/mutant
homodimers were insensitive to the T3 effect. As shown in
Fig. 3B
, ED/ED and ED/
TRß1 were dissociated by T3 in a
concentration-dependent manner. T3 also induced the
dissociation of OK/OK and OK/
TRß1 dimers (Fig. 3C
). For
quantitative comparison, the intensities of the dimer bands at each
concentration of T3 were quantified and plotted (Fig. 4
).
We have also included the previously reported dissociation curves of PV
homodimers and heterodimers for comparison (13). Examination of the
dissociation curves in Fig. 4I
shows that the ED50 for
T3-induced dissociation of
TRß1/
TRß1 was
virtually identical within experimental error (3.14.1
nM), irrespective of the presence of the type of mutant
(Table 3
). The ED50s for
T3-induced dissociation of ED/
TRß1 and OK/
TRß1
heterodimers were 48.5 ± 15 nM and 47.6 ± 12.9
nM, respectively; whereas no dissociation was detected for
PV/
TRß1 and S/
TRß1 at the T3 concentrations
examined (Table 3
). The mutant homodimers were less affected by
T3. However, at high T3 concentration (100
nM), approximately 10% and 50% of ED/ED and OK/OK
homodimers were dissociated from F2 (Fig. 4I
, B and C). But PV/PV and
S/S homodimers were not dissociated by T3 as high as 100
nM. Thus, these results indicate that the sensitivity of
T3-induced dissociation of F2-bound dimers correlates well
with the T3 binding affinities of the receptor in that the
ED50 is in the order of
TRß1<OK = ED<<S
= PV (see Tables 1
and 3
).

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Figure 3. Effect of T3 on the formation of TR
dimers. TRß1 homodimers, TRß1/S heterodimers, and S/S
homodimers (A); TRß1 homodimers, TRß1/ED heterodimers, and
ED/ED homodimers (B); TRß1 homodimers, TRß1/OK heterodimers,
and OK/OK homodimers (C). TRß1 homodimers, TRß1/wTRß1 and
wTRß1/wTRß1 homodimers (D). Equal amounts of TRß1 and mutant
(AC) or wTRß1 (D) were incubated with F2 (60 fmol) in the absence
or presence of T3 (1, 3, 6, 10, and 100 nM).
EMSA was carried out similarly as described in Fig. 1 .
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Figure 4. Quantative analysis of the F2-bound dimers. After
the gel was dried, the intensities of the TRE-bund dimeric bands were
quantified by PhosphoImager and plotted against the increasing
concentrations of T3. In 4I-A, wTRß1/wTRß1 (),
TRß1/ TRß1 ( ), TRß1/wTRß1 ( ); in 4I-AE,
TRß1/ TRß1 ( ), TRß1/mTR ( ), mTR/mTR ( ); in 4II
A-D, wTR 1/wTR 1 ( ), wTR 1/mTR ( ), mTR/mTR ( ); data are
expressed as mean ± SD (n = 3) with the
SD in the range of 515%.
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A more complex effect of T3 was seen for the binding
of wTR
1 and mutants to F2. As shown in Fig. 5A
, T3 induced not only the dissociation of wTR
1/wTR
1
homodimers, but also the dissociation of wTR
1/S heterodimers at the
T3 concentrations that had no effect on the stability of
F2-bound
TRß1/S dimers (Fig. 3A
vs. Fig. 5A
).
Interestingly, binding of the wTR
1 monomers was increasing while the
binding of wTR
1/wTR
1 and wTR
1/S were decreased by
T3. The effects of T3 on the binding of wTR
1
with mutant PV (Fig. 5B
), ED and OK (data not shown) were carried out
similarly. The ED50s were calculated from the
T3-induced dissociation curves shown in Fig. 4I
I. The
calculated ED50s shown in Table 3
indicate that the
ED50 for T3-induced dissociation of F2-bound
wTR
1/wTR
1 homodimers was 1.21.5 nM that was 2- to
3-fold lower than that for
TRß1/
TRß1 homodimers. The
ED50s were 20.7 ± 0.6, 33.1 ± 13.8, 11.4
± 2.6 and 11.4 ± 2.4 nM for T3-induced
dissociation of wTR
1/PV, wTR
1/S, wTR
1/ED and wTR
1/OK
heterodimers, respectively. These values were clearly much lower than
those for the corresponding
TRß1/M heterodimers. However, the
ED50s for ED/ED and OK/OK were higher than 100
nM that were similar to those derived when
TRß1 was
present. These results show that wTR
1, either as a homodimer or as a
heterodimer with mutant TR, was more sensitive to
T3-induced dissociation than
TRß1, indicating
isoform-dependent stability of F2-bound TRs in the presence of
T3. We have recently reported that wTR
1 binds to
T3 with a 3-fold higher affinity than wTRß1(Zhu,
X.-G., P. McPhie, K. H. Lin, and S. Y. Cheng, submitted for
publication). Taken together, this differential sensitivity correlates
with the T3-binding in that TR
1>TRß1>OK =
ED>>S = PV.
The potency of dominant negative action of PV on wTRß1 is higher
than on wTR
1
Previously we have shown that the potency of dominant negative
action of PV correlates well with the formation of TRß1/PV
heterodimers (13). The isoform-dependent differential T3
sensitivity of the wild-type/mutant heterodimers provided us a powerful
tool to further examine the role of wild-type/mutant heterodimers in
the dominant negative action of mutants. The analyses from the above
in vitro binding predicted that the dominant negative action
of a mutant on wTRß1 would be stronger than on wTR
1. To see if
this is the case, we carried out transient transfection assay in which
we assessed the potency of dominant negative action of PV by comparing
the transactivation activities of wTRß1 and wTR
1 in the presence
of PV. Figure 6A
shows that wTRß1 had a 2-fold higher
transactivation activity than wTR
1 (bars 8 vs. 4) that is
consistent with that reported previously (Zhu, X.-G., McPhie, P., Lin,
K.-H., and Cheng, S.-Y., submitted for publication). When PV expression
plasmid was cotransfected, the transactivation activity of wTRß1 and
wTR
1 was both suppressed (bars 6 and 10). However, the
transactivation activity of wTRß1 was suppressed nearly 2-fold more
by PV than of wTR
1 (Fig. 6B
). The similar extent of the dominant
negative action of PV on
TRß1 mediated by F2 (Fig. 6B
) further
supported the observations from the in vitro F2 binding in
that domain A/B has no effect on the activity of TRß1. Taken
together, these results indicate that the dominant negative action of a
mutant correlates with the stability of wild-type/mutant TR
heterodimers.
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Discussion
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We have investigated the mechanism of the dominant negative effect
of mutant TRs on the normal regulatory function of wild-type TRs, using
the interaction of four representative mutant proteins (PV, S, ED, OK)
with
TRß1 and wTR
1, in the presence of F2. Previously Yen
et al. (18) used a similar approach, studying the
interaction of another RTH mutant, Mf-1 (G345R), with wTRß1 and
wTR
1, again in the presence of F2. Because of the limitations of the
gel shift assay system, they were unable to resolve the various
DNA/protein complexes in their reactions. Using super shifting by
specific antibodies, they demonstrated the formation of both homo and
heterodimers, in 1:1 mixtures of mutant and wTRs with F2. In such a
mixture of Mf-1 and wTRß1, they observed that two-thirds of the DNA
bound proteins were released in the presence of 100 nM
T3. This is below the concentration range needed to release
isolated Mf-1 homodimers from F2 (EC50
500 nM; see Ref.16) and Mf-1 itself has no detectable affinity for T3 (19, 20). They interpreted this observation to indicate the release of both
TRß1/TRß1 and TRß1/Mf-1 dimers and concluded that only one of the
TRs in a heterodimer needs to bind T3, for dissociation
from DNA.
We took advantage of our recent observation that deletion of domain A/B
from wTRß1 in no way changes its affinity for T3 or for
TREs. However, the reduction in mol wt of
TRß1 makes it possible
to resolve homo and heterodimers formed on DNA binding with mutant
proteins by EMSA (13). Thus we can observe the specific behavior of
each species present in a mixture, rather than inferring its properties
from an average measurement. By studying mixtures of both wTR
1 and
TRß1, with four different naturally occurring mutant TRs, we have
obtained a clearer picture of the interactions of wild-type and mutant
TRs and their responses to increasing concentrations of
T3.
The results summarized in Table 2
show that, under the conditions of
our experiments, all dimers derived from
TRß1, composed of
wild-type and mutant proteins, have similar apparent affinities for F2
(Ka
1 x 109
M-1). The high concentrations of monomeric
complexes, observed in experiments using wTR
1, precluded a similar
simple analysis of that data. The constant ratios of homo and
heterodimers (1:3.5:1, wTR
1/wTR
1: wTR
1/mutant: mutant/mutant)
and the similar intensities of the bands in Figs. 1
and 2
, argue for a
similar conclusion in this case. The intrinsic affinity of the dimers
for F2 is independent of their composition.
However, the data shown in Fig. 4
and summarized in Table 3
demonstrate
that, in marked contrast, the response of any particular F2 bound dimer
to increasing concentrations of T3, is markedly influenced
by its composition. Homodimers of wTR
1 are more easily dissociated
by T3 than those of
TRß1. Heterodimers derived from
mutants ED and OK with
TRß1 are more stable than those derived
from wTR
1, whereas homodimers of these two mutants are only
partially dissociated. Homodimers of mutants PV and S, which have no
detectable affinity for T3, showed no dissociation over the
range of T3 concentrations that we investigated (0100
nM). The resistance of a dimer to dissociation from F2 by
T3, as measured by its ED50s, parallels the
reduction in the affinities for the hormone of both of its constituent
proteins (9, 10). This correlation strongly suggests that both
constituents of a TRE bound dimer must bind T3, before it
can dissociate. Thus, under physiological conditions, heterodimers
formed from wild-type and mutant TRs and wild-type homodimers will
respond very differently to increases in T3 concentration.
These heterodimers are therefore intimately involved in the dominant
negative action of the mutant TRs.
One puzzling observation in our experiments, which seems to argue
against this model, is the T3-induced dissociation of
heterodimers of PV and S with wTR
1, because these two mutants have
no detectable affinity for T3. However, a simple model
predicts that the efficacy of T3 to dissociate any given
dimer will depend on its affinity for both of the constituents of that
dimer. Thus, the relative concentration of wTR
1 homodimers will fall
rapidly with the second power of the hormone concentration. Because
wTRß1 has a lower affinity for T3, higher concentrations
of hormone will be required for full dissociation. Heterodimers of wTRs
with mutants ED and OK will show higher ED50s for
T3, reflecting very low affinities for hormone. In the
cases of mutants PV and S, the concentration of heterodimers will
decrease with only the first power of the hormone concentration,
yielding very high values of ED50, as observed.
If one assumes a similar thermodynamic equilibrium is to occur in
vivo, this would mean that at any given T3
concentration, there will be more wTRß1/mutant heterodimers bound to
F2 than wTR
1/heterodimers. Therefore, wTRß1/mutant heterodimers
can more effectively compete for binding to F2 than
wTR
1/heterodimers. Based on these considerations, we predicted that
the dominant negative action of a mutant on wTRß1 would be stronger
than on wTR
1. We tested this hypothesis by comparing the dominant
negative potency of PV on both TR isoforms. Indeed, we found that PV
had a approximately 2-fold higher dominant negative action on wTRß1
than wTR
1. Thus, one of the factors that dictate the dominant
negative potency of a mutant lies in the kind of the wild-type TR
heterodimer partner.
The present studies clearly demonstrate that mutants not only formed
heterodimers with TRß1, but with wTR
1. These heterodimers could
account for the dominant negative effect of the mutant receptors. When
equal amounts of wTRß1 and mutant receptors are present, the relative
contribution of inactive forms will be enhanced due to the binding of a
2-fold higher amount of wTRß1/mutant heterodimers and of
mutant/mutant homodimers to TREs, in competition with wTRß1
homodimers. It is reasonable to assume that a similar mechanism could
operate in RTH patients as it has been shown that nearly equal amounts
of normal and mutant TRß messenger RNA were found to be expressed in
some tissues of the RTH patients (21, 22). In addition, mutants can
also concurrently form inactive heterodimers with wTR
1 with binding
of a approximately 3-fold higher amounts of wTR
1/mutant heterodimers
to TRE, in competition with the wild-type homodimers. However, the
differential stability of wTRß1/mutant and wTR
1/mutant
heterodimers to T3 in the milieu added another additional
layer of regulation on the potency of dominant negative action.
However, it was reported that differential expression of normal and
mutant TRß messenger RNA could occur in the kindred (23). This,
together with the known differential expression of the wild-type
isoform TRs in different tissues (24, 25) will result in different
amounts of wild-type/mutant receptor heterodimers and mutant/mutant
homodimers that in turn could fine tune the dominant negative action of
the mutant receptors. Thus, the combinatorial diversities achieved via
complexes of wild-type and mutant receptor heterodimers and
mutant/mutant homodimers could contribute to the heterogeneity of
tissue resistances observed in RTH patients.
Received October 4, 1996.
 |
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