Environment-dependent long-range structural distortion in a temperature- sensitive point mutant
Transcript of Environment-dependent long-range structural distortion in a temperature- sensitive point mutant
Environment-dependent long-rangestructural distortion in a temperature-sensitive point mutant
Jannette Carey,1* Brian Benoff,2 Balasubramanian Harish,1
Lara Yuan,1 and Catherine L. Lawson2*
1Chemistry Department, Princeton University, Princeton, New Jersey 085442Department of Chemistry & Chemical Biology, Rutgers, The State University of New Jersey, Piscataway New Jersey 08854
Received 19 September 2011; Revised 25 October 2011; Accepted 27 October 2011DOI: 10.1002/pro.759Published online 4 November 2011 proteinscience.org
Abstract: Extensive environment-dependent rearrangement of the helix-turn-helix DNA recognition
region and adjacent L-tryptophan binding pocket is reported in the crystal structure of dimeric
E. coli trp aporepressor with point mutation Leu75Phe. In one of two subunits, the eight residuesimmediately C-terminal to the mutation are shifted forward in helical register by three positions,
and the five following residues form an extrahelical loop accommodating the register shift.
In contrast, the second subunit has wildtype-like conformation, as do both subunits in anisomorphous wildtype control structure. Treated together as an ensemble pair, the distorted and
wildtype-like conformations of the mutant apoprotein agree more fully than either conformation
alone with previously reported NOE measurements, and account more completely for its diversebiochemical and biophysical properties. The register-shifted segment Ile79-Ala80-Thr81-Ile82-Thr83
is helical in both conformations despite low helical propensity, suggesting an important structural
role for the steric constraints imposed by b-branched residues in helical conformation.
Keywords: hydrophobic brace; rotamer; cooperativity; crystal packing; ILV cluster
IntroductionThe tryptophan repressor of Escherichia coli (TrpR)
has served as an important early example of the
complexity of relationships among protein flexibility,
stability, and function. The TrpR dimer has extraor-
dinary thermal stability, unfolding cooperatively to
monomers in vitro with a midpoint temperature of
�92�C.1 Yet many complementary lines of experi-
mental evidence indicate that the helix-turn-helix
region (HtH) that contacts DNA is conformationally
mobile even in the presence of its ligands L-trypto-
phan and DNA. The earliest evidence came from
crystallographic studies showing that HtH helices D
and E (Fig. 1) can adopt different positions relative
to the dimeric protein core (helices A, B, C, and F of
both subunits), independent of L-tryptophan occu-
pancy.2 NMR studies by Jardetzky and coworkers3–7
demonstrated that segments D and E are helical in
solution on a nanosecond, but not a millisecond, time-
scale even in the presence of L-tryptophan. Thermo-
dynamic analysis of TrpR binding to L-tryptophan
and to DNA8 revealed very large heat capacity
changes, the signature of protein surface burial.9
Both crystallography and NMR showed that DNA
binding is accompanied by conformational adjustments
Additional Supporting Information may be found in the onlineversion of this article.
Brian Benoff current address is Middletown Board of Education,900 Nutswamp Road, Middletown, NJ 07748.Lara Yuan current address is Boston Biomedical Consultants,1000 Winter Street, Waltham, MA 02451.
Grant sponsor: NIH; Grant number: GM21589; Grant sponsor:National Science Foundation; Grant number: OISE0853423
*Correspondence to: Jannette Carey, Chemistry Department,Princeton University, Princeton, NJ 08544. E-mail: [email protected] or Catherine L. Lawson, Department ofChemistry & Chemical Biology, Rutgers, The State University ofNew Jersey, 610 Taylor Road, Piscataway, NJ 08854. E-mail:[email protected]
Published by Wiley-Blackwell. VC 2011 The Protein Society PROTEIN SCIENCE 2012 VOL 21:63—74 63
in HtH helices D and E.10,11 Further indications of
HtH mobility derive from proteolytic sensitivity in
helix D,12–14 molecular dynamics simulations,15–18 and
dramatic conformational rearrangement of the HtH
region in a domain-swapped crystalline TrpR gel.19
A genetic screen designed to identify mutations
conferring temperature-sensitivity in TrpR function
led to isolation of the point mutant L75F.20 In wild-
type (wt) TrpR, the partially solvent-exposed side-
chain of Leu75 at the C-terminus of helix D contacts
residues of the HtH and the dimeric core. Compared
to wt, the L75F mutant protein with Phe75 has
�10-fold weaker affinity for L-tryptophan, 2- to 5-
fold weaker affinity for operator DNA, and slight
increases in helix content and stability toward urea
denaturation.20 Although NMR spectra indicate that
the average solution structure of L75F apoTrpR
resembles wt apoTrpR, long-range effects on dynam-
ics are evident from significant changes in NOE pat-
terns and amide-proton exchange rates.20 Very large
NMR chemical-shift differences are detected for resi-
dues �25 A distant from Phe75, much too far away
to be ascribed to ring-current effects, and seemingly
inconsistent with the wt-like average solution struc-
ture.21 Measurements of apoTrpR backbone amide-
bond dynamics by 15N relaxation indicate that helix
D is more ordered in L75F than in wt, and that he-
lix E is less ordered.22
We initiated crystallographic study of the L75F
apoTrpR mutant to investigate the unusual biophys-
ical properties conferred by the L75F point muta-
tion. We report here the structure elucidation and
analysis of isomorphous crystals of L75F and wt
apoTrpR, which enable resolution of effects of the
L75F mutation from effects of crystal packing and
permit comparison with the NMR data.
Results and Discussion
Isomorphous wt and L75F apoTrpR
crystal structures
Structures of wt and L75F apoTrpR were obtained
from monoclinic crystals grown under identical con-
ditions and analyzed in parallel (see Methods). Each
structure consists of one complete homodimer with
two crystallographically independent subunits. Sum-
mary crystal, data collection, and refinement statis-
tics are provided in Table I.
In each structure the two subunit chains differ
strongly in relative order as judged by main-chain
atomic displacement parameters, particularly in
N-terminal arm and HtH regions [Fig. 2(A,B)]. The
nonequivalent HtH regions are designated here as
HtH1 and HtH2. The asymmetry is a consequence of
differences in local crystal packing environments
(Supporting Information Fig. S1). HtH1 has exten-
sive contacts with the N-terminal arm of a neighbor-
ing dimer, whereas HtH2 is largely free of crystal
contacts. The N-terminal arm-HtH1 contact buries
�900 A2 of total accessible surface area and resem-
bles the arm-HtH interaction between TrpR dimers
bound to DNA as well as interdimer contacts seen in
other TrpR crystal structures (Fig. 3). The relative
orientations of the interacting dimers and the extent
of arm-to-HtH contact differ considerably among
these structures, but in each case the N-terminal
arm Tyr7 phenol ring fills a shallow, largely hydro-
phobic depression lined by residues within or near
the HtH (Leu61, Leu62, Ser86, Leu89, Lys90, and
Arg97). The presence of arm-HtH interactions in mul-
tiple TrpR crystal structures lends strong support to
the suggestion that TrpR N-terminal arms mediate
higher-order association of dimers in solution.25–27
The two subunits of the wt dimer have nearly
identical conformations [Fig. 2(A)], but the two L75F
subunits differ substantially in the conformations of
their HtH regions [Fig. 2(B)]. The better-ordered
HtH1 of L75F [Fig. 2(B)] participates in the arm-
HtH tandem-like contact [Fig. 3(C)], (Supporting
Information Fig. S1) and has a wt-like fold. The more
poorly ordered HtH2 of L75F has a substantially
deformed helix E and D-E turn. Because the HtH2
region is relatively free of crystal contacts in both
Figure 1. wt holoTrpR,2 showing the arrangement of
helices (white subunit: A–F; dark subunit: a–f) and
L-tryptophan ligands (black sticks, dotted surface). Leu 75
lies within the DNA-binding helix-turn-helix region (white
subunit: D,E; dark subunit: d,e) and is shown as a skeletal
model indicated with black arrows. An interactive view is
available in the electronic version of the article.
64 PROTEINSCIENCE.ORG Long-Range Distortion Permitted by Point Mutation
structures, the altered conformation in the L75F
structure is likely a consequence of the mutation.
Comparison of wt and L75F HtH1 regions
Within the better-ordered HtH1 region the wt and
mutant structures are only subtly different from each
other. The Phe75 phenyl ring occupies the same posi-
tion as the Leu75 isobutyl group in the wt structure
[Fig. 2(C)]. Accommodation of the slightly longer,
bulkier Phe75 is achieved not locally but through a
�1 A rigid-body shift of the entire HtH1 [Fig. 2(C)].
The numerous contacts made by the side-chain of res-
idue 75 with residues of helix C are conserved.
The L-tryptophan binding site adjacent to HtH1
has a slightly larger pocket volume in L75F (316 A3;
see Methods) when compared with wt (302 A3), but
these are both much larger than in previously deter-
mined crystal structures for apoTrpR (178 A3) and L-
tryptophan-bound TrpR (246 A3).2,28 The variation in
L-tryptophan pocket volume results directly from flexi-
bility of the HtH helices, which adopt different posi-
tions in different crystal structures.2 Both wt and
L75F pockets contain partially ordered solvent. The
L75F binding site holds in addition a tris cation
((HOCH2)3CNH3þ) bound with partial occupancy; the
tris amino nitrogen and bulky central carbon sit
roughly at L-tryptophan a-amino nitrogen and a-car-
bon positions, respectively [compare Fig. 1 and Fig.
2(B)]. The presence of tris in only the L75F structure
suggests that the mutant may be more permissive
than wt to entry of molecular entities bulkier than the
native ligand. Although the binding of tris adjacent to
HtH1 is unique to the L75F structure, it is unlikely
that its presence influences HtH2 secondary structure,
since there is no cooperativity between the two L-tryp-
tophan binding sites of the TrpR dimer.8,20,29
Comparison of wt and L75F HtH2 regionsWithin the HtH2 region the two structures differ
more substantially. Helix D of the mutant is shifted
essentially as a rigid body by �3 A relative to wt
[Fig. 2(D)]. In addition, the residues that belong to
the interhelical turn and helix E in the wt structure
undergo a remarkable conformational change in the
mutant (Fig. 4). Residues 76–83 form an alternative
helix (E0) with the first turn in 310 conformation.
Mutant helix E0 occupies approximately the same
position as wt helix E residues 79–86; in other words,
the mutant helix is shifted out-of-register by three
residues relative to wt (Fig. 4). In the register-shifted
conformer, Ile82 takes the position occupied in wt by
Gly85. In the wt conformer the absence of a side-
chain at Gly85 accommodates the L-tryptophan
indole18,30; therefore, L-tryptophan binding would be
incompatible with the distorted mutant conformation.
In the mutant, the five residues following helix
E0 form a large loop, whereas in wt the same resi-
dues form the central part of helix E [Fig. 2(D)]. The
entire loop is heavily solvated and makes no crystal
contacts. The largest Ca-atom position shift between
wt and L75F structures is �10 A and is found in
this segment at Ser86, 11 residues distant in pri-
mary structure from the mutation site. The sequence
of loop residues 85–88, GlySerAsnSer, is turn-like
Table I. wt and L75F apoTrpR Crystal Structure Statistics
Space groupwt apoTrpR L75F apoTrpR
P21 P21
Unit cell lengths (A) a ¼ 35.7, b ¼ 54.3, c ¼ 56.9 a ¼ 35.7, b ¼ 54.1, c ¼ 55.6Unit cell angles (�) a ¼ 90, b ¼ 103.2, c ¼ 90 a ¼ 90, b ¼ 100.1, c ¼ 90Asymmetric unit content 2 subunits (1 dimer) 2 subunits (1 dimer)Solvent fraction 0.48 0.48Radiation source NSLS X26C NSLS X26CWavelength (A) 1.1 1.1Measured Reflections 176,611 103,879Unique reflections 24,536 28,206Resolution range (A) 50–1.67 (1.73–1.67) 50–1.58 (1.64–1.58)hI/ri 13.2 (4.5) 12.1 (5.5)Completeness 0.989 (0.948) 0.979 (0.877)Rmerge 0.066 (0.597) 0.073 (0.496)PDB id 3SSW 3SSXResolution range (highest resolution shell) (A) 24–1.67 (1.71–1.67) 27–1.58 (1.62–1.58)Reflections used in refinement 23,235 26,533Completeness for range (%) 93.8 92.4Rwork 0.176 (0.237) 0.176 (0.249)Rfree 0.219 (0.279) 0.219 (0.290)Protein atoms 1626 1684Solvent atoms 201 238RMS deviation, bonds (A) 0.02 0.02RMS deviation, angles (�) 1.49 1.79Residues with allowed f,w (%)a 100 100Residues with favored f,w (%)a 100 99.5
Carey et al. PROTEIN SCIENCE VOL 21:63—74 65
with low propensity for both helix and strand (Sup-
porting Information Fig. S3).
Residues 89–92 are in roughly the same position
and orientation in both mutant and wt structures,
forming the last turn of helix E in wt and a single-
turn helix (E00) in L75F. Mutant helices E0 and E00
are tip-to-tip and nearly coaxial (offset �30�). Atom
geometries and distances imply that the two seg-
ments are linked by a single helical-like backbone
hydrogen bond between Ile82 and Leu89, and by a
backbone hydrogen bond between Thr83 and Lys90
bridged by a water oxygen. Although the main-chain
conformation of Ser88 is extended beta rather than
helical, its carbonyl group makes the only i, i þ 4
backbone hydrogen bond within helix E00, to the
Ala92 amide. The Ser88 side-chain hydroxyl oxygen
can also form a hydrogen bond with the Ala91 am-
ide, providing an N-terminal cap31 for the short E00
helix. There are no side-chain interactions between
helices E0 and E00 instead, residues of both helical
segments participate in hydrophobic contacts with
residues of surrounding helices as discussed further
below.
Resolving effects of crystal contacts
and mutationThe dramatic difference in conformations of the two
chains of the L75F mutant apoTrpR dimer raises the
question of whether the distortions in HtH2 arise
from mutation or from crystal packing. When the
two HtH regions are superimposed on each other
within the context of the crystal lattice, the rela-
tively open environment of the deformed HtH2
appears to offer no steric hindrance to adoption of
the wt-like conformation. A refinement test designed
to investigate the possibility that wt-like conforma-
tion might be adopted by at least a small percentage
of L75F apoTrpR dimers at the HtH2 position within
the crystal gave a clear negative result (see Meth-
ods). In contrast, the relatively restrictive HtH1
Figure 2. Comparison of isomorphous apoTrpR crystal structures. (A) wt apoTrpR and (B) L75F apoTrpR are displayed in
ribbon representation with colors reflecting main-chain atomic displacements (<25 A2: dark blue; >55 A2: red). The two
independent helix-turn-helix regions are indicated as HtH1 and HtH2. Black arrows and skeletal side-chains indicate L75F
point mutation positions. A tris cation occupying one L-tryptophan binding pocket in the L75F apoTrpR structure is also
shown (compare dotted surface for tris in (B) and for L-tryptophan in Fig. 1). In (C) and (D), HtH regions of the two structures
are shown overlaid after overall least-squares fit of all dimer Ca atoms. (C) HtH1 (wt: gray; L75F: cyan with selected residue
labels and Phe 75 in magenta). (D) HtH2 (as in panel C except L75F is colored orange). An interactive view is available in the
electronic version of the article.
66 PROTEINSCIENCE.ORG Long-Range Distortion Permitted by Point Mutation
lattice environment, which includes the tandem-like
arm-HtH contact, cannot accommodate the deformed
conformation owing to severe clashes. These obser-
vations indicate that the HtH conformation of the
L75F mutant depends on the environmental context,
i.e., whether or not there is contact with a neighbor-
ing dimer in the crystal lattice. Analogously, the
HtH2 lattice environment of wt apoTrpR offers no
steric hindrance to adoption of a distorted conforma-
tion. Thus, the conformational difference between wt
and mutant HtH2 conformations can be attributed
directly to the L75F mutation.
To better understand how the L75F mutation
enables the conformational change, side-chain pack-
ing interactions in the apoTrpR structures were ana-
lyzed. The two alternative packing arrangements
can be described as differing in the register of the
helical Ile79-Ile82 segment relative to invariantly
Figure 3. TrpR N-terminal arm-HtH interactions in (A) tandem trpR-DNA complex crystal structure (PDBid 1trr),23 (B) TrpR
crystal structure (PDBid 1wrp),28 (C) apoTrpR crystal structure (this work; PDBid 3ssw). Each panel shows a pair of trpR
dimers involved in an arm-HtH interaction (HtH: green subunit; arm: orange subunit; in the tandem complex only (panel A), a
second symmetry-related arm-HtH interaction is also shown). In the top half of each panel, the first (blue/green) dimer view
orientation is held constant to highlight the range of positions occupied by the second (orange/pink) dimer; Pro6 and Tyr7
residues of the N-terminal arm are displayed in red on each subunit (L-trp: black; DNA: thin wire). In the bottom half of each
panel, details are shown for each interaction, with arm residues Pro6 and Tyr7 (carbon: orange; nitrogen: blue; oxygen: red)
and interacting HtH residues (carbon: green; nitrogen: blue; oxygen: red). In apoTrpR (panel C), an arm-HtH interaction is
made only to HtH1; although a second N-terminal arm (green subunit) is proximal to HtH2 (orange subunit), it is not visible in
electron density at Pro6, Tyr7 positions. The local environment difference between HtH1 and HtH2 provides an explanation for
the selective permissiveness to conformational change observed in the isomorphous L75F mutant structure. Arm-HtH
interactions closely similar to those seen in the tandem trpR-DNA complex (A) are also observed in a tetragonal crystal form
of holoTrpR24 (structure not shown; PDBid 1ZT9).
Figure 4. Structure-based sequence alignment of distorted L75F and wt subunits. Residues 57–93 of each 107-residue
subunit are shown with helix assignments. Boxes enclose residues in helical conformation as judged by main-chain f,wangles. Gray shading indicates 310-helix conformation. Lower-case denotes residues in turns. Dots indicate positions usually
occupied by hydrophobic residues in helix-turn-helix DNA binding proteins28 (‘‘hydrophobic brace’’).
Carey et al. PROTEIN SCIENCE VOL 21:63—74 67
positioned residues of the L-tryptophan binding
pocket: Ile57 and Val58, which are located in the
C-terminal half of helix C, and Leu89, located near
the C-terminus of helix E or within helix E00 (Fig. 5).
In wt and wt-like mutant conformations, Leu/Phe75
and helical residues Thr81 and Ile82 pack against
Ile57 [Fig. 5(A,B)]. In the distorted mutant conforma-
tion, the helix-register shift and 310 conformation
result in Ile79 occupying the wt position of Ile82, and
Ile82 occupying the wt position of Gly85 [Fig. 5(C)].
In the distorted conformation only, Ile79 joins the
cluster of packed residues. Thus, the alternative pack-
ing of two segments with relatively invariant local
structures, 79–82 and 57–58, links the burial of Ile79
to the looping out of residues 84–88 from helix E.
As expected, the solvent-accessible surface areas
of the two packing arrangements differ significantly.
When the whole chain or only the HtH regions are
considered, the distorted conformer of apo L75F
TrpR buries slightly less hydrophobic as well as total
surface area than the wt-like conformer, and both
conformers bury slightly more surface area than wt
apoTrpR (Supporting Information Table S1). How-
ever, when only the alternatively packed b-branched
segments are considered, the distorted L75F con-
former has hydrophobic and total surface area burial
that is approximately 2-fold more efficient than wt
or wt-like L75F. Although the crystal structures
indicate that both conformations are accessible to
L75F apoTrpR, the enhanced local surface burial of
L75F may explain why the distorted conformation is
favored for the mutant in the absence of crystal con-
tacts. Differences in solvent-accessible surface areas
cannot be used directly to assess the relative stabil-
ities of the two conformers because crystallization is
an inherently hysteretic process and thus crystal
structures need not reflect equilibrium distributions
of conformers. On the other hand, because the differ-
ences in structure between the two conformers of
L75F are strictly local, and appear to be controlled
by the alternative packing of these b-branched seg-
ments, the relative stabilities of the two conformers
may also reflect the local packing efficiency of these
segments rather than the global packing efficiency.
Comparison with NMR dataNMR data for L75F TrpR clearly indicate the long-
range nature of the effects of the L75F mutation.
Although early NMR spectra were fully consistent
with a wt-like average structure, the number of
NOESY cross-peaks was much larger than in wt
spectra acquired under the same conditions.20
ROESY spectra ruled out spin diffusion as a trivial
cause of the NOESY results.20 The rate of deuterium
exchange of unresolved amide protons was �50%
slower than in wt, as were exchange rates for the
resolved indole protons of both Trp19 and Trp99.20
All of the proton exchange data were adequately fit
by single-exponential decay functions, indicating
generally similar rate-limiting steps for exchange in
the wt and mutant proteins. Two well-resolved,
slowly-exchanging amide protons were detected in
1D spectra of the mutant only, as well as a promi-
nent NOESY crosspeak between them20; these were
later assigned to Met42 and Leu43 in the B-C
turn.21 In addition, a prominent HSQC crosspeak
unique to the mutant was detected20 that was later
assigned to the Thr44 amide.21
Full assignment of L75F apoTrpR21 revealed
extremely large chemical shift changes for residues
up to �26 A from Phe75, far too distant to be
explained by effects of the ring current of the new
aromatic residue. Furthermore, many distant resi-
dues were very strongly shifted while others closer
to the mutation site were not. Among amide nitro-
gens assigned in both mutant and wt, the largest15N chemical shift differences were found for Thr81,
Ile82, and Thr83, which shift upfield by 2.03, 3.90,
Figure 5. Alternative side-chain packing in the L75F apoTrpR mutant. (A) wt apoTrpR (B) L75F apoTrpR, wt-like subunit (C)
L75F apoTrpR, distorted subunit. In all three panels, side-chains of selected residues are represented as space-filling models;
the backbone is represented as a white tube. The indole ring position of the L-trp binding site is indicated in (A) and (B) as a
semitransparent gray surface (in front of G85, V58, and L89 in this view). The side-chain for Thr81, discussed in the main text,
was omitted from the images for clarity. In panel A and B views, Thr81 sits directly in front of Ile82.
68 PROTEINSCIENCE.ORG Long-Range Distortion Permitted by Point Mutation
and 4.42 ppm, respectively; the largest shifts for
assigned amide nitrogens closer to the mutation site
are 1.32 ppm upfield for Asn73 and 1.75 ppm down-
field for Gly76. For comparison, the distances from
Phe75 to each of these residues on the wt-like side
of the L75F crystal structure reported here are
Thr81, 10.4 A; Ile82, 10.2 A; Thr83, 14.0 A; Asn73,
5.9 A; and Gly76, 3.8 A. Examples of residues that
are similarly distant from Phe75 as residues 81–83
but experience little or no change in chemical shift
include Gly78, 8.7 A, �0.17 ppm; and Glu70, 8.3 A,
�0.08 ppm. The chemical-shift results in the L75F
HtH region were previously rationalized as reflecting a
global response to the mutation with effects at nearby
residues complicated by ring-current shifts.21 The ring
current was assumed to extend as much as 10 A from
Phe75 to include potential anisotropic effects. Never-
theless, very significant 15N chemical-shift changes
(�1–2 ppm upfield for backbone amides) as distant as
�28 A away in the same subunit and �26 A away in
the other subunit could not be explained.
The average NMR structure of L75F apoTrpR
derived from NOESY restraints is very similar to
that of wt TrpR, as are all the individual members
of the family of accepted structures.21 Like all NMR
structures of TrpR solved to date, the dimeric core of
L75F apoTrpR (helices A, B, C, and F) is well-
constrained by the data. In contrast, considerable
variation in the HtH regions of L75F was attributed
to instability of these domains, following the inter-
pretation of more extensive data available for wt
apoTrpR.3,5 When compared with the dimeric core,
the L75F and wt HtH regions share a general pau-
city of NOEs, limited protection of amides from
exchange, and smaller chemical-shift deviations
from random coil, indicating that they are much less
well-defined. However, other NMR measures indi-
cate apparently more helical structure for the HtH
of L75F than for wt. L75F residues 67–83 have
several i, i þ 3 NOEs and two i, i þ 4 NOEs between
a-carbon and backbone amide protons that are
absent in wt, as well as larger helical chemical shift
deviations for a-carbons and a-protons.21 These data
provide the restraints that result in models for L75F
apoTrpR that are more helical in the HtH region
than corresponding models for wt.
Although the environment-dependent distortion
in the L75F crystal structure suggests that both con-
formations might also occur in solution, none of the
HtH region conformations in the family of accepted
NMR solution structures for L75F apoTrpR (PDB id
2xdi)21 closely resembles either conformation in the
crystal structure. This finding prompted evaluation
of both wt-like and distorted conformations against
NOE-based distance restraints. Of 728 measured
NOEs, only ten conflict with either one or both crys-
tal structure conformations, with inferred interpro-
ton distances that are too long to generate an NOE
of the measured strength (Table II). Significantly,
the discrepancies are not found throughout the mol-
ecule but involve exclusively residues involved in
the alternative packing depicted in Figure 5. Many
of these discrepancies do involve residues relatively
close to the Phe75 aromatic ring, but ring-currents
that can affect chemical shift positions do not affect
relaxation processes such as NOEs.
Of the 10 identified NOEs, five are consistent
with the distorted conformation but inconsistent
with wt-like conformation. In particular, two strong
NOEs with upper limit distances of 4.5 A from Ile79
to Gly76 and to Ala77 are much better accounted for
by the distorted structure. Conversely, 2 of the 10
NOEs are fully consistent with wt-like conformation
but inconsistent with distorted conformation. Thus,
neither structure alone can account for all the data.
The final 3 of the 10 NOEs involve residue pairs
Phe75-Ala80, Gly76-Ile79, and Asn87-Leu89; neither
wt-like nor distorted conformations have interproton
distances sufficiently short to satisfy the correspond-
ing restraints. However, an intermediate conforma-
tion representing a transition between the two crys-
tallographic conformations might reasonably be
expected to bring each of these residue pairs into
sufficiently close proximity to yield an NOE.
NOE strength, though proportional to distance,
is not necessarily proportional to population or dura-
tion; thus, NOEs can over-represent transitory close
encounters. Indeed, van Gunsteren32 has developed
an approach that uses NOE-derived restraints as
time-averaged bounds. In this method the ensemble as
a whole satisfies all the observed NOEs, rather than
the conventional treatment that requires every struc-
ture in the ensemble to satisfy all restraints. If the
HtH region of L75F apoTrpR alternates between two
conformations in solution, each conformation would
account for only some of the NOEs, and the structure
calculated by the conventional approach would not
reflect these dynamics, but present only an apparently
disordered region. This situation appears to best
account for the NMR results on L75F apoTrpR.
Reanalysis of NMR evidence for L75F apoTrpR
thus suggests that more than one conformation
must be populated in solution to account for all the
data. The highly nonuniform patterns of NMR
changes include those that are predicted if the dis-
torted crystal conformer of L75F were present in
solution. A recent analysis of 15N backbone relaxa-
tion data for L75F apoTrpR22 indicates that the
spin–spin relaxation of Ile82 is strongly affected by
an exchange process, supporting the existence of a
conformational transition involving the HtH region.
The relaxation data also indicate enhanced flexibil-
ity for residues 84–88 in L75F relative to wt. The
picture that emerges is that in solution, L75F
apoTrpR samples conformations that likely include
both conformations observed in the crystal structure.
Carey et al. PROTEIN SCIENCE VOL 21:63—74 69
The transition between the two crystallographic con-
formations could be accomplished by relatively mod-
est chain excursions compared with conversion to
the domain-swapped gel form that both wt and L75F
TrpR undergo.19
In addition to accounting for NOEs in the imme-
diate vicinity of the mutation, the presence of the
distorted structure in solution would provide a
highly satisfactory explanation for the effects
detected by NMR involving the distant amide groups
of Met42, Leu43, and Thr44. In wt apoTrpR and the
wt-like side of L75F apoTrpR, these residues are
closely approached by the guanidinium group of
Arg84, whereas in the distorted L75F conformation
the looping-out of segment 84–88 between helices E0
and E00 moves Arg84 away and brings several
uncharged residues nearby (Thr81, Ile82, Ser86,
Asn87). This change represents a substantial pertur-
bation of the electronic environment that could read-
ily affect nearby amide protons. Furthermore, since
Leu43 methyl protons display NOEs to Trp19 indole
ring protons, the change might be responsible for
the large chemical shift changes experienced by all
the hydrophobic residues on the Trp19 face of helix
A in the L75F mutant, as well as the blue-shifting of
the fluorescence emission spectrum attributed to
Trp19 (see discussion below).20 All of these puzzling
perturbations detected at so many residues far
removed from the site of mutation have not other-
wise been explained by any NMR structures or
relaxation analyses conducted to date.
Comparison with biophysical data
A large body of data that has accumulated on L75F
apoTrpR can be partly rationalized by the structures
and analysis reported here.
The urea denaturation midpoint monitored by
circular dichroism (CD) is slightly higher than for
wt (�7.0 M vs. �6.5 M), but the thermal midpoint
assessed by differential scanning calorimetry (�91�C)
is unaltered.20 The heat capacity change upon dena-
turation is similar to that of wt (�90 kcal/mol), and
the ratio of van’t Hoff to calorimetric enthalpy is near
one for both proteins, indicating a two-state unfolding
process.20 These data are consistent with the general
picture of TrpR as a highly stable but reversibly fold-
ing dimer.33,34 The interdependent tertiary and qua-
ternary organization of the intertwined central core
is expected to be relatively insensitive to structural
changes in the more peripheral HtH DNA-binding
domains, consistent with local control of HtH stability
based on the packing data. The independence of the
HtH domains from the central dimer fold is dramati-
cally illustrated by the finding that chymotrypsin
cleavage of wt apoTrpR dimers within the HtH yields
four fragments that reassociate spontaneously to
regenerate the native NMR spectrum.14
Although apoTrpR stability is largely unaltered
by the L75F mutation, the CD spectrum shows an
increase in helix content compared to wt from �77
to �85% of residues.20 However, the structures show
that WT apoTrpR has two more residues in helical
conformation than the distorted conformer, in appa-
rent opposition to the CD results, although the effects
of helix length and distortion can complicate interpre-
tation of the fraction of helical residues.35 On the
other hand, the increased helical CD intensity and
slightly higher resistance to urea denaturation are
consistent with the modest improvement in relative
order seen in the crystal (Fig. 2). Both proteins reach
�87% helix content upon titration with trifluoroetha-
nol,20 implying that even in the absence of cosolvent
L75F TrpR has nearly the maximal helix content per-
mitted by its primary structure. Only the domain-
swapped crystalline gel formed by wt or L75F TrpR
in isopropanol has higher helix content (�89% as cal-
culated from the structure), due to conversion of the
C-D and D-E turns to helical conformation.19
Table II. Comparison of NOEs and Inferred Interproton Distances for L75F apoTrpR
NOEs Inferred H-H distancesL75F apoTrpR in solutiona L75F apoTrpR crystal structureb
Proton 1 Proton 2NOE distanceupper limit (A)
wt-likeconformation (A)
Distortedconformation (A)
Phe 75 Hb Ile 79 Hc2 6.5 11.8–14.5 4.5–5.9Phe 75 Hd1 Ile 79 Hc2 8.3 11.9–13.5 7.9–8.5Gly 76 H Ile 79 Hb 4.5 12.2 4.4Gly 76 Ha Ile 79 H 5.5 8.7–9.6 4.8–5.1Ala 77 Ha Ile 79 H 4.5 6.5 3.7Ile 57 Hc2 Thr 81 Hc2 5.5 3.6–6.6 6.7–9.9Phe 75 H Ala 77 Hb 6.0 4.6–6.3 8.8–9.6Phe 75 Hb Ala 80 Hb 6.5 11.5–13.5 8.4–9.8Gly 76 H Ile 79 Hc1 5.5 10.4–11.4 6.4–7.2Asn 87 Ha Leu 89 Hd1 6.7 7.1–9.3 8.5–11.5
a NOE restraints for PDB id 2xdi.21
b Interproton distances or distance ranges were measured between predicted hydrogen atom positions in the L75F apoTrpRcrystal structure (PDB id 3SSX). Bold ranges indicate values consistent with the observed NOE.
70 PROTEINSCIENCE.ORG Long-Range Distortion Permitted by Point Mutation
The intensity-weighted fluorescence emission max-
imum is blue-shifted by �2.3 nm in L75F apoTrpR rela-
tive to wt, mainly due to changes at the red edge of the
spectrum, with an overall increase in intensity of
�14%.20 With excitation at 280 nm, emission is con-
fined almost entirely to the two native Trp residues at
positions 19 and 99. Based on analysis of the NMR
results,21 the spectral changes could be assigned to an
altered electronic environment at Trp19 despite its
being �25 A away from Phe 75 in the same subunit and
�15 A away in the other subunit in wt conformation.
However, the distorted conformation of L75F better
explains the fluorescence results as reflecting the prox-
imity of Trp19 to Leu43 in the L-trp binding pocket,
where the electronic environment is strongly affected
by the alternating proximity of Arg84. The altered L-trp
binding affinity of L75F20 is also consistent with occlu-
sion of the binding pocket by the distortion.
Significance of b-branched residuesin helical segments
In the course of comparing the 20 accepted NMR
structures of L75F apoTrpR with the crystal struc-
ture reported here, the isolated HtH regions of the
forty subunits of the NMR models and the two crys-
tal subunits were superimposed on each other inde-
pendently of their positions with respect to the dimer
core. Residues 80–82 were found to adopt a highly sim-
ilar conformation in all structures. This result was
unexpected considering the limited set of NMR con-
straints available in the HtH region, and prompted a
more detailed evaluation based on the variation in
main-chain phi, psi angles in these structures (Sup-
porting Information Fig. S4). The variation in main-
chain conformation is high in turns and low in helical
regions, with the notable exception of the HtH region.
Helix E residues 83–89 present almost as much varia-
tion as do turn regions, but residues 80–82 are nearly
as invariant as helical residues of the dimeric core,
with phi, psi angle values near the helical minimum
on the Ramachandran plot. Thus, even though the
wide distribution of HtH conformations in the family
of NMR structures implies apparent instability of this
region, residues 80–82 appear to have intrinsic helical
order. This finding is consistent with the alternative
packing patterns in the crystal structure in which this
helical segment appears to move as a unit.
The seemingly high degree of helical order for
residues 80-82 is also unexpected given their local
sequence environment, as they are embedded within
a segment rich in b-branched and Gly residues:
76-GlyAlaGlyIleAlaThrIleThr-83. This sequence has
relatively low helical propensity (Supporting Infor-
mation Fig. S3). The occurrence of b-branched resi-
dues in helical segments is entropically disfavored
because their side-chains can access only one
rotamer conformation due to steric hindrance
between the bulky Cb branch point and the helical
backbone.36 In principle, the steric hindrance could
be relieved by unraveling of the segment into a more
extended structure, but the resulting excursion of
the chain might compromise tertiary interactions. A
similar argument can be made regarding residues
76-GlyAlaGlyIle-79, which adopt 310-helix conforma-
tion in the distorted L75F apoTrpR subunit. Their
side-chains offer minimal steric hindrance that
would promote extension of the helix rise from a- to
310 conformation, and this sequence also has overall
low helical propensity (Supporting Information Fig.
S3). The fact that it adopts 310 conformation rather
than a-helix or random coil is consistent with a role
for tertiary constraints. Tertiary constraint of sec-
ondary structure was invoked to explain why addi-
tional residues inserted within helical segments of
lysozyme are accommodated not by helix lengthen-
ing but by displacement of adjacent helical residues
into flanking turn regions.37 The coupling of second-
ary and tertiary structures is thought to be the
molecular origin of protein folding cooperativity.38
In TrpR, the tertiary interactions made by the
b-branched residues of helix E or E0 involve Ile57
and Val58, which are within a segment of helix C
that is also rich in b-branched residues, 53-ThrArg-
ValArgIleVal-58. Thus, the distortion and register
shift of the E0 helix act together to accommodate the
en bloc movement of one b-branched segment (79–
83) while maintaining efficient packing with another
b-branched segment (53–58) that preserves its con-
formation. The participation of b-branched residues
in tertiary constraint calls to mind the transmem-
brane helix of glycophorin A,39 in which such residues
play a key role at the quaternary level as well.
b-branched residues are common in helical segments of
membrane proteins, and have been thought to reflect
altered helical propensity in the membrane environ-
ment.40 However, the bilayer acts as a constraint on he-
lix length and on helix–helix packing through its influ-
ence on the exposure of polar and nonpolar residues to
the surrounding lipid, analogous to the tertiary con-
straint in soluble proteins. Helical b-branched residues
present side-chains that are preorganized for interac-
tion with intra- or intermolecular partners, making
them perhaps ideally suited to enforce super-secondary
constraints whether these arise from the tertiary struc-
ture in the case of soluble proteins or the bilayer in the
case of membrane proteins.
Sigler and coworkers had earlier coined the
term ‘‘hydrophobic brace’’ to describe the interactions
between residues in these b-branched-rich segments
because they appeared to fix the intrinsic conforma-
tion of the HtH motif and its orientation relative to
the rest of the molecule in TrpR as well as in several
other HtH repressors.28 In Figure 4, brace residue
positions are indicated by dots. Mutation of Leu75 to
Phe crowds the brace, resulting in rearrangement as
reflected in the alternative packing arrangements
Carey et al. PROTEIN SCIENCE VOL 21:63—74 71
shown in Figure 5. Rearrangement of the brace to
accommodate the mutation implies that the brace is
not a rigid enforcing structure as its name suggests,
but rather is adaptable. The majority of brace resi-
dues in Sigler’s group of repressors are Ile, Leu, and
Val, all of which in addition to being hydrophobic
have severe restrictions on their side-chain confor-
mations. The present analysis thus suggests that a
more complete definition of the brace would high-
light steric constraints on conformational mobility.
Clusters of the branched aliphatic side-chains
Ile, Leu, and Val (ILV) have recently been implicated
as early organizing features of both native and off-
pathway folding intermediates of TIM barrel and
Rossmann fold proteins.41 In native proteins ILV
clusters appear to correlate with regions in which
backbone amides are highly protected from hydrogen
exchange, an effect that has been ascribed to the sol-
vent-excluding property of the branched side-chains
that shields the underlying backbone.42,43 Residues
Val55, Ile57, Val58, and Ile82 from the b-branched
segments of helices C and E, as well as Leu75 from
helix D, belong to the ILV cluster of wt TrpR (S.
Kathuria and C. R. Matthews, personal communica-
tion). However, the backbone amides of both Leu75
and Ile82 are among the most rapidly exchanging in
wt apoTrpR.4 Thus, cluster residue Ile82 is unlikely
to contribute to the apparently intrinsic helical char-
acter of the 80–82 segment of helix E by a solvent-
exclusion mechanism, supporting a role for steric hin-
drance. It is worth noting that even Leu, though not
b-branched, has significant steric restriction that may
contribute to the role of ILV clusters. In the rotamer
library of Dunbrack and Karplus,36 only 2% of the
Leu chi1 conformers lie in the range 60� 6 60�; the
remainder are divided about 2:1 between the other
two conformers, regardless of backbone conformation.
The relative importance of steric hindrance and sol-
vent exclusion in ILV clusters may be resolvable with
a larger database of protein hydrogen-exchange rates.
Conclusions
The crystal structures of isomorphous wt and L75F
apoTrpR that are reported here reveal considerable
perturbation in the L-tryptophan-binding and DNA-
binding HtH region caused by the Leu to Phe substi-
tution. In crystals of the L75F mutant the extent
and nature of structural distortion depend on local
environmental context: an extensive crystal lattice
interaction at one HtH supports a wt-like conforma-
tion, whereas the other HtH lacking crystal contacts
presents a major rearrangement of secondary and
tertiary structure. Given that (i) the lattice interac-
tion supporting the wt-like conformation of L75F
involves an N-terminal arm-HtH contact that is also
likely to be relevant in solution, and (ii) the dis-
torted HtH conformation largely lacks crystal con-
tacts, it is likely that both conformations observed in
the crystal are sampled by L75F apoTrpR in solu-
tion. Inclusion of the these conformers within the
family of accepted NMR structures of L75F apoTrpR
provides a more fully satisfactory explanation of all
existing biophysical and NMR data. The results indi-
cate that distinct alternative conformations can be
overlooked despite full NMR structure determina-
tion as well as detailed relaxation measurements.
Without structural models of specific alternative con-
formers to guide analysis, NMR data may appear to
indicate poor ordering of a segment.
Experimental Procedures
Crystallization and data collectionwt and L75F apoTrpR were purified as described.20,44
Protein stocks were stored frozen at �12 mg/mL in
250 mM NaCl, 0.1 mM PMSF, 0.1 mM sodium phos-
phate, pH 7.0, at �20�C prior to crystallization trials.
Crystals were obtained by standard hanging-drop
vapor diffusion at 294 K with Hampton Research Crys-
tal Screen condition #6 (30% (w/v) PEG 4000, 200 mM
MgCl2, 100 mM Tris HCl pH 8.5). Single crystals grew
overnight with typical dimensions 0.2 mm � 0.2 mm �0.05 mm. One wt apoTrpR crystal and one L75F
apoTrpR crystal were soaked for 30 s in Hampton
Research crystal screen cryo condition #6 (24% (w/v)
PEG 4000, 180 mM MgCl2, 80 mM Tris HCl, pH 8.5,
and 20% (v/v) glycerol), mounted on nylon loops, and
flash-cooled to 100 K in a N2 gas stream. X-ray dif-
fraction data were collected at the Brookhaven
National Laboratory National Synchrotron Light
Source beamline X26C with an ADSC Quantum 4
CCD detector. The incident radiation wavelength was
1.1 A. Reflections were integrated, scaled, and merged
using HKL2000.45 Data collection statistics are pro-
vided in Table I.
Structure determination
Initial phases were obtained for both wt and L75F mu-
tant structures by the molecular replacement method
using the program AMORE.46 In each case the search
model was orthorhombic TrpR dimer2 (PDBid 2oz9),
with L-tryptophan ligands and solvent excluded. Rota-
tion and translation solutions were unambiguous. Each
structure was subjected to multiple cycles of refinement
and manual model-building using Phenix47 and
COOT.48 Atomic displacements were modeled with indi-
vidual isotropic B-factors and a single set of transla-
tion-libration-screw (TLS) parameters for all atoms.
Analysis and displayConformation occupancy test: a composite L75F
apoTrpR model was constructed with residues 74–95
from the HtH2 chain in both wt-like and deformed
conformations, each initially at half occupancy. The
model was subjected to refinement against the X-ray
diffraction data for occupancy only, with no solvent
72 PROTEINSCIENCE.ORG Long-Range Distortion Permitted by Point Mutation
model imposed. The occupancy of the deformed con-
formation increased to 0.95, while the occupancy of
the wt-like conformation decreased to 0.07, indicat-
ing that wt-like conformation is not present in the
HtH2 region of the L75F structure.
The Molprobity server49 was used to evaluate
main-chain conformation, as reported in Table I; the
Molprobity server was also used to add hydrogen
atoms to the crystal structures for comparison of the
L75F apoTrpR crystal structure with NOE restraint
data. Each proton–proton distance was measured and
compared to the cutoff distance assigned on the basis
of the strength of each NOE, taking into account dis-
tance ambiguities for chemically equivalent protons.
L-tryptophan ligand pocket volumes were meas-
ured using the Castp server.50 Because the position
of the Arg84 side-chain varies significantly between
the models compared, the calculations were per-
formed on models in which Arg84 side-chain atoms
beyond Cb were removed.
Secondary structure propensities (Supporting In-
formation Fig. S3) were determined using four differ-
ent propensity scales as follows. Stapley-Doig a: DGvalues for residue in helix relative to residue in coil.51
Stapley-Doig b: DG values for residue in b-strand rela-
tive to Ala in b-strand.51 Minor-Kim b: DDG values for
residue in b-strand relative to Ala in b-strand.52 Pace-
Scholtz a: DDG values for the residue in a-helix rela-
tive to Ala in a-helix.53 For each propensity scale, val-
ues for individual residues were summed and the sum
divided by the number of residues in the segment.
Variance of main-chain torsion angles phi and
psi (Supporting Information Fig. S4) in the 20 L75F
apoTrpR NMR model chains and two X-ray crystal
structure model chains were calculated using Pro-
check-NMR.54
Calculations of accessible surface area (Support-
ing Information Table S1) used the program NAC-
CESS.55 The solvent probe was a water molecule of
1.4 A radius, and the slice size (Z-step) was 0.05 A.
Graphical images were created using Pymol56
(Figs. 1–3, 5, and Supporting Information Fig. S1) and
UCSF Chimera57 (Supporting Information Fig. S2).
Acknowledgments
We thank M. Gryk, G. Rose, and C. Yanofsky for valua-
ble discussions, S. Kathuria and C.R. Matthews for
bringing ILV clusters to our attention and for applying
their analysis to TrpR, G. Montelione for advice on
comparing NOEs to calculated distances, V. Copi�e for
providing the ensemble of models of the L75F apo-trpR
mutant minimized against NMR restraints prior to
their deposition and the NMR relaxation results prior
to publication, and A. Heroux for assistance with data
collection at National Synchrotron Light Source beam-
line X26C, which is supported by the Department of
Energy and the National Institutes of Health (NIH).
References
1. Bae SJ, Chou WY, Matthews K, Sturtevant JM (1988)Tryptophan repressor of Escherichia coli shows unusualthermal stability. Proc Natl Acad Sci USA 85:6731–6732.
2. Lawson CL, Zhang RG, Schevitz RW, Otwinowski Z,Joachimiak A, Sigler PB (1988) Flexibility of the DNA-binding domains of trp repressor. Proteins 3:18–31.
3. Arrowsmith C, Pachter R, Altman R, Jardetzky O(1991) The solution structures of Escherichia coli trprepressor and trp aporepressor at an intermediate reso-lution. Eur J Biochem 202:53–66.
4. Czaplicki J, Arrowsmith C, Jardetzky O (1991) Seg-mental differences in the stability of the trp-repressorpeptide backbone. J Biomol NMR 1:349–361.
5. Zhao D, Arrowsmith CH, Jia X, Jardetzky O (1993)Refined solution structures of the Escherichia coli trpholo- and aporepressor. J Mol Biol 229:735–746.
6. Gryk MR, Finucane MD, Zheng Z, Jardetzky O (1995) So-lution dynamics of the trp repressor: a study of amide pro-ton exchange by T1 relaxation. J Mol Biol 246:618–627.
7. Zheng Z, Czaplicki J, Jardetzky O (1995) Backbone dy-namics of trp repressor studied by 15N NMR relaxa-tion. Biochemistry 34:5212–5223.
8. Jin L, Yang J, Carey J (1993) Thermodynamics of ligandbinding to trp repressor. Biochemistry 32:7302–7309.
9. Spolar RS, Record MT, Jr. (1994) Coupling of local fold-ing to site-specific binding of proteins to DNA. Science263:777–784.
10. Otwinowski Z, Schevitz RW, Zhang RG, Lawson CL,Joachimiak A, Marmorstein RQ, Luisi BF, Sigler PB(1988) Crystal structure of trp repressor/operator com-plex at atomic resolution. Nature 335:321–329.
11. Zhang H, Zhao D, Revington M, Lee W, Jia X, Arrow-smith C, Jardetzky O (1994) The solution structures ofthe trp repressor-operator DNA complex. J Mol Biol238:592–614.
12. Tsapakos MJ, Haydock PV, Hermodson M, SomervilleRL (1985) Ligand-mediated conformational changes inTrp repressor protein of Escherichia coli probedthrough limited proteolysis and the use of specific anti-bodies. J Biol Chem 260:16383–16394.
13. Carey J (1989) trp repressor arms contribute bindingenergy without occupying unique locations on DNA.J Biol Chem 264:1941–1945.
14. Tasayco ML, Carey J (1992) Ordered self-assembly ofpolypeptide fragments to form nativelike dimeric trprepressor. Science 255:594–597.
15. Komeiji Y, Uebayasi M, Someya J, Yamato I (1991) Mo-lecular dynamics simulation of trp-aporepressor in asolvent. Protein Eng 4:871–875.
16. Guenot J, Kollman PA (1992) Molecular dynamics stud-ies of a DNA-binding protein. II. An evaluation ofimplicit and explicit solvent models for the moleculardynamics simulation of the Escherichia coli trprepressor. Protein Sci 1:1185–1205.
17. Howard AE, Kollman PA (1992) Molecular dynamicsstudies of a DNA-binding protein. I. A comparison ofthe trp repressor and trp aporepressor aqueous simula-tions. Protein Sci 1:1173–1184.
18. Komeiji Y, Fujita I, Honda N, Tsutsui M, Tamura T,Yamato I (1994) Glycine 85 of the trp-repressor of E.coli is important in forming the hydrophobic trypto-phan binding pocket: experimental and computationalapproaches. Protein Eng 7:1239–1247.
19. Lawson CL, Benoff B, Berger T, Berman HM, Carey J(2004) E. coli trp repressor forms a domain-swappedarray in aqueous alcohol. Structure 12:1099–1108.
Carey et al. PROTEIN SCIENCE VOL 21:63—74 73
20. Jin L, Fukayama JW, Pelczer I, Carey J (1999) Long-range effects on dynamics in a temperature-sensitivemutant of trp repressor. J Mol Biol 285:361–378.
21. Tyler R, Pelczer I, Carey J, Copie V (2002) Three-dimensional solution NMR structure of Apo-L75F-TrpR, a temperature-sensitive mutant of the trypto-phan repressor protein. Biochemistry 41:11954–11962.
22. Goel A, Tripet BP, Tyler RC, Nebert LD, Copie V (2010)Backbone amide dynamics studies of Apo-L75F-TrpR, atemperature-sensitive mutant of the tryptophanrepressor protein (TrpR): comparison with the (15)NNMR relaxation profiles of wild-type and A77V mutantApo-TrpR repressors. Biochemistry 49:8006–8019.
23. Lawson CL, Carey J (1993) Tandem binding in crystalsof a trp repressor/operator half-site complex. Nature366:178–182.
24. Joachimiak A, Schevitz RW, Kelley RL, Yanofsky C, SiglerPB (1983) Functional inferences from crystals of Esche-richia coli trp repressor. J Biol Chem 258:12641–12643.
25. Chae YK, Abildgaard F, Royer CA, Markley JL (1999)Oligomerization of the EK18 mutant of the trprepressor of Escherichia coli as observed by NMR spec-troscopy. Arch Biochem Biophys 371:35–40.
26. Mackintosh SG, McDermott PF, Hurlburt BK (1998)Mutational analysis of the NH2-terminal arms of thetrp repressor indicates a multifunctional domain. MolMicrobiol 27:1119–1127.
27. Vangala S (1998) Protein folding and protein-proteininteractions: exploring issues of function and bioavaila-bility. Madison: University of Wisconsin.
28. Zhang RG, Joachimiak A, Lawson CL, Schevitz RW,Otwinowski Z, Sigler PB (1987) The crystal structureof trp aporepressor at 1.8 A shows how binding trypto-phan enhances DNA affinity. Nature 327:591–597.
29. Arvidson DN, Bruce C, Gunsalus RP (1986) Interactionof the Escherichia coli trp aporepressor with its ligand,L-tryptophan. J Biol Chem 261:238–243.
30. Schevitz RW, Otwinowski Z, Joachimiak A, Lawson CL,Sigler PB (1985) The three-dimensional structure oftrp repressor. Nature 317:782–786.
31. Richardson JS, Richardson DC (1988) Amino acid pref-erences for specific locations at the ends of alpha heli-ces. Science 240:1648–1652.
32. Torda AE, Scheek RM, van Gunsteren WF (1990) Time-averaged nuclear Overhauser effect distance restraintsapplied to tendamistat. J Mol Biol 214:223–235.
33. Gittelman MS, Matthews CR (1990) Folding and stabil-ity of trp aporepressor from Escherichia coli. Biochem-istry 29:7011–7020.
34. Mann CJ, Royer CA, Matthews CR (1993) Tryptophanreplacements in the trp aporepressor from Escherichiacoli: probing the equilibrium and kinetic folding mod-els. Protein Sci 2:1853–1861.
35. Sreerama N, Venyaminov SY, Woody RW (1999) Esti-mation of the number of alpha-helical and beta-strandsegments in proteins using circular dichroism spectros-copy. Protein Sci 8:370–380.
36. Dunbrack RL, Jr., Karplus M (1993) Backbone-depend-ent rotamer library for proteins. Application to side-chain prediction. J Mol Biol 230:543–574.
37. Heinz DW, Baase WA, Dahlquist FW, Matthews BW(1993) How amino-acid insertions are allowed in analpha-helix of T4 lysozyme. Nature 361:561–564.
38. Carey J, Lindman S, Bauer M, Linse S (2007) Protein recon-stitution and three-dimensional domain swapping: benefitsand constraints of covalency. Protein Sci 16:2317–2333.
39. MacKenzie KR, Prestegard JH, Engelman DM (1997) Atransmembrane helix dimer: structure and implica-tions. Science 276:131–133.
40. Li SC, Deber CM (1994) A measure of helical propen-sity for amino acids in membrane environments. NatStruct Biol 1:368–373.
41. Hills RD, Jr., Kathuria SV, Wallace LA, Day IJ, BrooksCL, 3rd, Matthews CR (2010) Topological frustration inbeta alpha-repeat proteins: sequence diversity modu-lates the conserved folding mechanisms of alpha/beta/alpha sandwich proteins. J Mol Biol 398:332–350.
42. Wu Y, Vadrevu R, Kathuria S, Yang X, Matthews CR(2007) A tightly packed hydrophobic cluster directs theformation of an off-pathway sub-millisecond folding in-termediate in the alpha subunit of tryptophan syn-thase, a TIM barrel protein. J Mol Biol 366:1624–1638.
43. Kathuria SV, Day IJ, Wallace LA, Matthews CR (2008)Kinetic traps in the folding of beta alpha-repeat pro-teins: CheY initially misfolds before accessing thenative conformation. J Mol Biol 382:467–484.
44. Joachimiak A, Kelley RL, Gunsalus RP, Yanofsky C,Sigler PB (1983) Purification and characterization oftrp aporepressor. Proc Natl Acad Sci USA 80:668–672.
45. Otwinowski Z, Minor W, Processing of X-ray diffractiondata collected in oscillation mode. In: Carter CW, SweetRM, Eds. (1997) Methods in enzymology, Vol. 276. SanDiego: Academic Press, pp 307–326.
46. Navaza J (2001) Implementation of molecular replace-ment in AMoRe. Acta Crystallogr D Biol Crystallogr57:1367–1372.
47. Adams PD, Afonine PV, Bunkoczi G, Chen VB, Davis IW,Echols N, Headd JJ, Hung LW, Kapral GJ, Grosse-Kuns-tleve RW, McCoy AJ, Moriarty NW, Oeffner R, Read RJ,Richardson DC, Richardson JS, Terwilliger TC, ZwartPH (2010) PHENIX: a comprehensive Python-based sys-tem for macromolecular structure solution. Acta Crystal-logr D Biol Crystallogr 66:213–221.
48. Emsley P, Lohkamp B, Scott WG, Cowtan K (2010)Features and development of Coot. Acta Crystallogr DBiol Crystallogr 66:486–501.
49. Chen VB, Arendall WB, III, Headd JJ, Keedy DA,Immormino RM, Kapral GJ, Murray LW, RichardsonJS, Richardson DC (2010) MolProbity: all-atom struc-ture validation for macromolecular crystallography.Acta Crystallogr D Biol Crystallogr 66:12–21.
50. Dundas J, Ouyang Z, Tseng J, Binkowski A, Turpaz Y,Liang J (2006) CASTp: computed atlas of surface topog-raphy of proteins with structural and topographicalmapping of functionally annotated residues. NucleicAcids Res 34:W116–W118.
51. Stapley BJ, Doig AJ (1997) Free energies of amino acidside-chain rotamers in alpha-helices, beta-sheets andalpha-helix N-caps. J Mol Biol 272:456–464.
52. Minor DL, Jr., Kim PS (1994) Measurement of thebeta-sheet-forming propensities of amino acids. Nature367:660–663.
53. Pace CN, Scholtz JM (1998) A helix propensity scalebased on experimental studies of peptides and proteins.Biophys J 75:422–427.
54. Laskowski RA, Rullmannn JA, MacArthur MW, Kap-tein R, Thornton JM (1996) AQUA and PROCHECK-NMR: programs for checking the quality of proteinstructures solved by NMR. J Biomol NMR 8:477–486.
55. Hubbard SJ, Thornton JM (1993) ‘NACCESS’, Com-puter Program, Department of Biochemistry and Mo-lecular Biology, University College London.
56. Delano WL (2002) The Pymol molecular graphics sys-tem. Palo Alto: Delano Scientific.
57. Pettersen EF, Goddard TD, Huang CC, Couch GS,Greenblatt DM, Meng EC, Ferrin TE (2004) UCSF Chi-mera—a visualization system for exploratory researchand analysis. J Comput Chem 25:1605–1612.
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