Results
Substitution of conserved amino acids in loop1 decrease catalytic activity
The influence of loop1 sequence on HisF function was assessed by mutational analysis. First,
a multiple sequence alignment (MSA) was compiled which revealed that most residues within
loop1 are highly conserved ( Figure 2A ), indicating a function of this loop in the catalytic
mechanism. To test this hypothesis, conserved residues were replaced by either alanine,
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proline, or glycine. Whereas alanine substitutions should uncover effects based on
electrostatic or hydrophobic interactions, proline or glycine substitutions were introduced to
reveal effects related to loop mobility. The assumption was that introduction of proline residues
would render loop1 more rigid in the detached state, whereas inclusion of glycine residues
would increase loop1 mobility. The resulting HisF loop1 variants were expressed in E. coli,
purified, and characterized by steady-state enzyme kinetics. The determined turnover numbers
(kcat) and Michaelis constants for PrFAR (KMPrFAR) are listed in Table 1.
Figure 2: Sequence conservation and mutational analysis of loop1. (A) Sequence logo (generated
with WebLogo3.6) based on a multiple sequence alignment (MSA) of about 1300 HisF sequences.
Residues are numbered according to HisF from T. maritima. Mutated residues are marked with white
arrows. Residues whose mutation to Ala, Pro, or Gly resulted in a significant reduction of catalytic activity
are marked with orange arrows. ( B) Detailed view of the open loop1 conformation (PDB ID: 1VH7 38).
Functionally important residues within loop1 are shown as orange sticks or spheres. Residue F38 is
marked in yellow sticks, the catalytic residues D11 and D130 are shown as blue sticks. (C) Detail view
of the closed loop1 conformation (PDB ID: 7AC840, chain E). The bound substrate analogue ProFAR is
shown in stick representation (colored by element).
Table 1: Steady state kinetic parameters of wt-HisF and loop1 variants at 25 °C.
kcat
(s-1)
KMPrFAR
(µM)
kcat/KMPrFAR
(M-1 s-1)
wt 2.4 ± 0.2 4.5 ± 0.5 5.3 x 105
K19A 1.1 ± 0.1 6.1 ± 1.8 1.8 x 105
G20A 2.2 ± 0.1 x 10-2 2.1 ± 0.2 1.0 x 104
G20P n.d. n.d. -
T21G 1.8 ± 0.1 x 10-2 5.0 ± 0.8 3.6 x 103
T21P n.d. n.d. -
N22A 2.9 ± 0.2 x 10-1 8.4 ± 1.7 3.4 x 104
F23A 5.5 ± 0.4 x 10-3 6.8 ± 1.3 8.1 x 102
E24P n.d. n.d. -
L26A 1.1 ± 0.03 2.0 ± 0.3 5.5 x 105
D28A 2.4 ± 0.1 4.5 ± 0.9 5.3 x 105
G30A 1.0 ± 0.1 x 10-1 3.7 ± 1.3 2.7 x 104
G30P n.d. n.d. -
F38A 2.3 ± 0.1 3.5 ± 0.6 6.6 x 105
wt CouA 1.5 ± 0.1 4.1 ± 0.9 3.7 x 105
n. d.: no activity detectable.
Values ± SE for kcat and KMPrFAR were determined by fitting with equations 1 and 2 of the mean for
technical triplicates.
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While some importance has been attributed to the residue corresponding to K19 in the
homologous yeast enzyme His752, we did not observe significant loss of activity for the K19A
variant. Likewise, the amino acid substitutions L26A and D28A did not affect catalytic activity.
However, most of the substitutions (G20A, N22A, F23A, G30A, T21G) resulted in a significant
decrease of the kcat value, whereas the KMPrFAR values did not differ by more than two -fold in
comparison to wt-HisF. The most severe effects were observed for the proline substitutions
(G20P, T21P, E24P and G30P) which caused a drop of catalytic activity belo w the detection
limit. The relatively constant KMPrFAR values and the dramatically decreased kcat values imply
that loop1 does not contribute significantly to the energetics of substrate binding, but rather
plays a role for catalysis. As there are no indications that loop1 residues are directly involved
in acid-base catalysis, loop1 must play an indirect role in substrate turnover. To obtain insights
into this role we have concentrated on three of the identified HisF variants that likely modulate
the conformational landscape of loop1. First, the HisF-F23A variant was selected to enhance
the flexibility of loop1. This variant will likely destabilize both the closed and open
conformations as F23 stacks onto the PrFAR ligand in the closed state and interacts with F38A
to form the open state (Figure 2B, C). Second, the HisF-G20P variant was selected to restrict
conformational flexibility of loop1 in the detached state . At the same time, this variant will
destabilize the closed conformation as residue 20 is part of a β -strand in that state ( Figure
2C). Finally, the HisF-F38A variant was selected. It contains a mutation outside loop1 and is
intended to destabilize the open conformation without effecting the closed conformation.
Whereas the G20P and F23A substitutions decrease the kcat of wt-HisF by several orders of
magnitude, the F38A substitution has no effect on the steady-state catalytic parameters (Table
1).
Amino acid substitutions shift the populations of the loop1 conformations
To assess whether the mutations have an influence on the conformation of loop1 we
determined the structures of the HisF-F23A and HisF-G20P variants by X-ray crystallography.
In the crystal, the HisF -G20P variant was found in the open conformation, similar as the wt -
HisF protein (Figure S1A). For the HisF-F23A variant the electron density for residues 20-24
in loop 1 was lacking, indicating that the conformation of loop1 shifted from the open towards
the detached state (Figure S1B).
To complement these static crystal structures, we subjected the wt -HisF, as well as the
variants HisF -F23A, HisF -G20P, and HisF -F38A, to a limited proteolysis analysis. This
experiment should provide insights into the conformational mobility of the proteins, since
protease cleavage rates depend on the accessibility of the respective target 53-54 and it has
been shown previously, that trypsin specifically cleaves HisF after R27 in loop1. 34 In our
experiments we observed that wt-HisF and the variant HisF-F38A are cleaved at similar rates.
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The HisF-F23A variant, on the other hand, was cleaved faster, whereas the HisF-G20P variant
displayed a reduced cleavage rate (Figure 3A). These results are in accordance with the static
structures that we solved and that suggested a shift towards the mobile detached state for the
HisF-F23A variant and a stably formed open conformation for the HisF-G20P variant.
To obtain direct information on the flexibility of loop1, we exploited NMR experiments. First,
we made use of heteronuclear NOE (hetNOE) measurements that probe structural fluctuations
on the ps-ns timescale.55 These fast motions result in {1H}-15N hetNOE values below 0.7. For
the wt-HisF protein we found that loop1 is the most dynamic loop in the protein. This implies
that loop1 predominantly occupies the detached state in solution. It should, however, be noted
that the open state of loop1 is also sampled as deletion of loo p1 results in chemical shift
perturbations in residues that interact with loop1 in the open state. To assess the effect of the
mutations on the conformation of loop1 we compared {1H}-15N hetNOE values of wt-HisF with
those of the variants HisF-F38A, HisF-F23A, and HisF -G20P (Figure 3B-D). This revealed
that the structural flexibility of loop1 is increased in HisF-F23A variant and, to a small degree,
in variant HisF -F38A. These findings confirm that loop1 spends more time in the detached
state when the open state is destabilized by the F23A and F38A mutations. By contrast, the
ps-ns dynamics of loop1 in the HisF -G20P variant is slightly reduced, in agreement with an
increased stability of the open state and thus a shift in the conformation away from the
detached state.
Figure 3: Amino acid substitutions change flexibility and ps -ns dynamics of loop1. (A) Limited
proteolysis assays monitoring the rates of trypsin cleavage at loop1 residue R27 for wt-HisF, HisF-F38A,
HisF-F23A, and His-G20P. Cleavage patterns observed immediately after addition of trypsin (0 min) and
after incubation at 25°C for 20 min and 200 min are visualized by SDS polyacrylamide gel
electrophoresis (PAGE) analysis. (B, C, D) {1H}-15N hetNOE values of wt-HisF (blue) in comparison to
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loop1 variants (orange) HisF -F38A (B), HisF-F23A (C) and HisF -G20P (D). Decreased values in the
loop1 region (residues 19-30) of HisF-F38A and HisF-F23A in comparison to wt-HisF reveal increased
dynamics on the ps to ns timescale. The loop dynamics of the HisF -G20P is slightly decreased
compared to the wt-HisF.
We further supplemented our analysis with molecular dynamics (MD) simulations of wt -
HisF and the HisF-G20P, HisF-F23A and HisF-F38A variants, in both the unliganded state and
in complex with PrFAR. In the case of the unliganded enzyme, as there is no exper imental
evidence for loop closure in this state, we initiated trajectories only from the loop1 -open
conformation of the enzyme. However, in the case of the PrFAR-bound enzymes, we initiated
simulations from both the open and closed states of loop1 for completeness.
Figure S2 shows the root mean square fluctuations (RMSF) of all Cα-atoms of HisF during
MD simulations of the different systems studied. These reflect the flexibility of loop1 (residues
19-30) in wt -HisF and how this is impacted by the mutations. This figure shows only subtle
differences in loop1 flexibility among the loop variants: however, given that the loop is highly
flexible in all variants, the relative flexibility of the loop will not necessarily change, although
there may be shifts within that ensemble between open, detached , and closed states . We
further note that the large absolute value of the loop1 RMSF obtained in the simulations of the
PrFAR-bound enzymes initiated from the loop1 closed conformation ( Figure S2B) is due to
conformational adjustment of the loop to a new (but still closed) conformation (Figure S3),
likely due to the change in ligand from ProFAR present in the crystal structure ( Figure 1) to
the substrate PrFAR (see Materials and Methods).
In order to explore the impact of mutations on loop1 flexibility in the different loop states in
more detail, we examined the relative mobilities of loop1 based on this RMSF analysis (Figure
4). The mobility data is supplemented by a projection of loop1 motion in wt-HisF along the first
principal component, PC1, from principal component analysis (PCA) of these MD simulations
to illustrate the dominant dynamic motif. From this data, it can be seen that the relative mobility
profiles vary depending on enzyme variant in simulations initiated from the open conformation
of loop1 (in both the unliganded and PrFAR bound states of the enzyme, see Figures 4A and
B), with much more subtle differences in simulations initiated from the PrFAR -bound loop-
closed conformation (Figure 4C). This is due to the high mobility of loop1 in all variants, as our
simulations shift the loop towards a new closed conformation. We note also that in simulations
initiated from the closed state of loop1, we observe a clear monomodal distribution of mobilities
in all variants, peaking towards the center of the loop. In contrast, loop mobility is more complex
(and variant dependent) in simulations initiated from the loop1 open conformations, likely due
to the loop changing shape as it samples both open and detached conformations.
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Figure 4: Relative mobility of loop 1 during MD simulations. The mobilities were calculated from the
RMSF of the loop1 C α-atoms, as outlined in the Supplemental Methods. Shown here are data from
analysis of simulations of the (A) unliganded simulations initialized from the loop1 open conformation,
and of simulations of the PrFAR -bound enzymes initialized from the loop1 ( B) open and (C) closed
conformations. For comparison, panels ( D-F) show projections of the first principal component, PC1,
from principal component (PCA) analysis of these simulations (performed as described in the
Supplemental Methods) onto representative structures of the ( D) open unliganded, (E) open PrFAR
bound, and (F) closed PrFAR bound states of wt -HisF. The color gradient indicates the transition of
loop1 along this principal component.
Finally, to further analyze the flexibility of loop1, we constructed 2D histograms of loop1
motion as a function of the root mean square deviations (RMSD) of the C α-atoms of loop1
relative to the closed conformation observed in the crystal structure of wild -type HisF/HisH in
complex with ProFAR ( PDB ID: 7ac840, chain E and F ), and the distance RMSD of all non-
covalent interactions in the loop1 open conformation of the loop (PDB ID: 1THF48) projected as
a single vector. The corresponding data is shown in Figures 5, alongside snapshots illustrating
the conformational space sampled by loop1 in each set of simulations, colored by C α-atom
RMSF of loop1. From this data, it can be seen that in both unliganded and liganded simulations
(Figure 5), we sample both open and detached state (the latter show up as a “smear” on the
histograms, as this state is very mobile). The relative population of these states is then shifted
by the introduction of point mutations on the loop. In the case of the F38A and F23A variants,
we see a clear shift towards more detached states dominating our simulations, but not in the
case of the G20P variant. This shift is also illustrated in the enlarged 1D histograms of the
dRMSD from the open state contacts (y -axis of the 2D plot), where the histogram of low
dRMSD values is decreased for F23A and F38A and increased for G20P. This is in agreement
with (and confirming) the observations from our {1H}-15N hetNOE experiments (Figure 3).
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Figure 5: Conformational ensemble of loop1 during molecular dynamics simulations of
unliganded and PrFAR-bound wt-HisF, HisF-F38A, HisF-F23A, and HisF-G20P. Shown in
the middle of the figure are 2D-histograms of the root mean square deviations (RMSD) of the Cα-atoms
of loop1 relative to the crystal closed structure of wild-type and the distance RMSD of all non-covalent
interactions in the loop1 that stabilize open liganded conformation during simulations of unliganded (left
side) and PrFAR-bound systems (right side). Regions corresponding to closed and open conformations
are indicated with a circle. Enlarged 1D histograms of the distance RMSD are included along with the
2D-histograms for the simulations without a ligand. For details of how the distance RMSD values were
calculated, see the Supplemental Methods. The panel on the left shows, from top to bottom, snapshots
of loop1 motion in wt-HisF, HisF-F38A, HisF-F23A, and HisF-G20P during the unliganded simulations,
colored by the Cα-atom RMSF of loop1 . The panel on the right shows the analogous data from our
corresponding PrFAR-bound MD simulations (variants presented in the same order).
Furthermore, in our simulations of the liganded enzyme (Figure 5), where we also included
the closed state of the loop in our simulations, we observe only sparse sampling of this closed
state in the F23A and G20P variants compared to the corresponding sampling of the closed
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state in the F38A variant and the wild-type enzyme. A comparison of Ramachandran plots for
glycine and proline in wt-HisF and HisF-G20P (Figure S4) shows that angles of G20 sampled
in our simulations of wild-type closed or closed active conformations are forbidden by proline
Ramachandran plot, explaining why the closed state is so destabilized for the HisF -G20P
variant. The impaired sampling of a catalytically competent closed conformation in these
variants helps rationalize the diminished/abolished activity observed for these variants in the
kinetic data (Table 1).
In summary, our crystallography, proteolysis, NMR, and simulation data demonstrate that
the HisF-G20P and HisF-F23A variants have opposing effects on the conformation of loop1.
In both the HisF -G20P and HisF-F23A variants, there is a shift away from the closed
conformations in our simulations, with preferred sampling of detached or open states of the
loop. However, whereas loop1 primarily samples the open conformation in the HisF -G20P
variant, the loop1 p opulation shifts towards the highly flexible detached conformation in the
HisF-F23A variant. As these variants both strongly reduce catalytic turnover (Table 1), it is not
possible to link the population of open and detached conformations of loop 1 with the rate-
limiting step ( kcat) in the turnover reaction. Instead, the G20P and F23A substitutions likely
influence turnover via alterations in the closed conformation of loop1.
Amino acid substitutions in loop1 have a limited effect on substrate binding affinities
Since different loop1 conformations in the apo state cannot explain the higher catalytic
activities of wt -HisF and HisF -F38A compared to HisF -G20P and HisF -F23A, it was next
analyzed whether these amino acid substitutions have consequences for substrate or product
binding. To study the thermodynamics and kinetics of PrFAR binding to HisF, fluorescence
equilibrium titrations and transient fluorescence kinetic measurements were performed.
Although intrinsic fluorescence of the single tryptophan residue 156 of HisF has previously
been used as spectroscopic signal transmitter in ligand binding studies45, it proved unsuitable
for kinetic measurements because of the unspecific fluorescence quenching upon addition of
the substrate PrFAR. We sought to avoid this effect by the introduction of an alternative
fluorescent probe. The unnatural amino acid L -(7-hydroxycoumarin-4-yl)ethylglycine (CouA)
was applied because this probe is relatively small, has good spectroscopic properties and can
easily be introduced by genetic code extension. 56-57 CouA has been used extensively as
protein-based fluorescent sensor that reports on protein-ligand interactions56, 58-60 and enzyme-
substrate binding.61-62 As the 7-hydroxycoumarin moiety can exist in a number of tautomeric
forms in the ground state, absorption/emission maxima are strongly influenced by
environmental factors such as dielectric constant, hydration and pH.63 For our purposes CouA
was incorporated into HisF in place of a lysine at position 132, a position that is not conserved
in HisF sequences and has a distance of ~ 15 Å to the ligand binding site ( Figure 6A). HisF-
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K132CouA variants (wt, F38A, F23A, G20P) were purified with reasonable yields and the
incorporation of CouA was verified spectroscopically ( Figure S 5). Steady -state kinetic
parameters of CouA -labeled HisF were virtually identical to those of its non -labelled
counterpart (Table 1), corroborating that enzymatic activity is not affected by incorporation of
the fluorophore. Ligand binding is associated with a decrease of CouA fluorescence emission.
Equilibrium titrations with the substrate PrFAR were done in the absence of ammonia to allow
for observation of the binding separately from the turnover reaction (Figure 6B).
Figure 6: Ligand binding monitored by equilibrium titrations with CouA-labelled HisF. (A) Site of
CouA incorporation. The structure of HisF is shown with the open loop1 conformation (orange, PDB
entry 1vh738) and an overlay of the closed loop1 conformation (beige, PDB entry 7ac8 40). CouA was
modelled into the structure and is shown at position 132 (within β -strand 5) as cyan sticks, the bound
substrate precursor ProFAR and the catalytic residues D11 (within β-strand 1) and D130 (within β-strand
5) are shown as sticks. (B) Equilibrium titrations of HisF-CouA variants at 25°C. Binding of the substrate
PrFAR to the variants (0.2 µM) resulted in a decrease in CouA fluorescence ( lex = 370 nm, lem = 452
nm). Relative emission intensity was plotted vs. PrFAR concentration. Lines represent hyperbolic fits of
the data. (C) Apparent KD values obtained in equilibrium titrations for the binding of the substrate PrFAR
or the product molecules ImGP and AICAR to the HisF -CouA variants in absence or presence of the
second ligand (AICAR or ImGP), respectively. The associated numerical values are listed in Table S1.
KD values ± SE were determined by fitting the mean ± SEM for at least two technical replicates w ith
equation 3.
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The KD-values determined in the equilibrium titrations show that the G20P and F23A
substitutions in loop1 slightly weaken the affinity between HisF and the substrate PrFAR or the
products ImGP or AICAR (Figure 6C, Table S 1). For example, compared between wt -HisF
and HisF-F23A the dissociation constant for the substrate PrFAR is increased 1.8 -fold, for
ImGP 1.2-fold, and for AICAR 1.4 -fold. Furthermore, we noticed that the apparent affinity of
AICAR is slightly increased in the presence of the second ligand ImGP and vice versa, which
indicates a higher formation propensit y of the ternary complex (HisF*ImGP*AICAR) in
comparison to the respective binary complexes (HisF*AICAR) and (HisF*ImGP). The
stabilization effect due to formation of the ternary complex is similar for wt -HisF and HisF -
G20P, HisF-F23A, and HisF -F38A, indicating that this is a general feature. Looking at the
fluorescence changes upon titration of the dimeric or ternary complexes, another difference
between wt-HisF/His-F38A and HisF-F23A/HisF-G20P is noticeable. While the fluorescence
amplitudes in the case o f HisF-wt and HisF -F38A are higher when the ternary complex is
formed than when the binary complexes are formed, the opposite is true for the variants HisF-
F23A and HisF -G20P ( Table S 2). This is a first indication that the environment of the
fluorophore CouA in the ternary complex for the active variants wt-HisF and HisF-F38A differs
from the environment in the inactive variants HisF-F23A and HisF-G20P.
An induced-fit movement during PrFAR binding is exclusively observed for wt-HisF and
HisF-F38A
The kinetics of the PrFAR binding reaction were studied in stopped-flow experiments, whereby
the CouA fluorescence decrease was recorded after rapidly mixing the respective HisF-CouA
variant with a molar excess of PrFAR. For an assessment of ligand binding kinetics, the
observed binding transients were fitted with exponential functions. The number of exponential
functions required to describe the transients allows conclusions to be drawn about the number
of reaction steps in the binding reaction. In additio n, the secondary plots derived from
exponential fitting, e.g. kobs as function of the PrFAR concentration, provide initial clues to the
binding mechanism. In general, time traces (Figure S6) for wt-HisF and HisF-F38A resemble
each other, whereas time traces associated with the loop1 variants HisF-F23A and HisF-G20P
showed notable differences. In the case of wt -HisF ( Figure S 6A) and variant HisF -F38A
(Figure S6B) time traces are biphasic (sum of two exponential terms ). A fast fluorescence
decrease is followed by a slow phase with a very small signal amplitude. In the case of loop
variants HisF-F23A (Figure S6C) and HisF-G20P (Figure S6D), single exponential functions
were adequate to describe the time traces. The overall fluorescence changes associated with
PrFAR binding were smaller, which resulted in lower signal-to-noise ratios. A plot of the first-
order rates (kobs) for the binding reaction as a function of PrFAR concentration provides insights
into potential differences in the binding mechanisms of the different variants. In the case of wt-
HisF and HisF -F38A, the turnover rate ( kobs1) depends on the substrate concentration in a
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hyperbolic manner (Figure S6E), indicating that binding takes place via an induced fit or
conformational selection mechanism.64-65 In contrast, in the case of loop1 variants HisF-F23A
and HisF-G20P, kobs, increased linearly with increasing concentrations of PrFAR (Figure S6F),
which is indicative of a simple binding process without involvement of conformational changes.
This finding is in accordance with a model where the wt-HisF and HisF-F38A proteins bind the
ligand when the protein is in the open or detached conformation, after which loop1 stably
closes over the li gand to form the closed conformation. The HisF -G20P and HisF -F23A
variants on the other hand are unable to form a stably closed conformation and prefer to remain
in the open or detached conformation even in the presence of the ligand, as also observed in
our simulations (Figures 5).
To directly assess if the formation of the closed state is impaired in the HisF -G20P and
HisF-F23A variants we again turned to NMR titration experiments. To that end, we added
ProFAR (a stable PrFAR analogue; see Figure 1A), to 15N labelled HisF and followed the
induced chemical shift perturbations (CSPs). For all HisF proteins we observed CSPs that
directly report on the interactions between HisF and the ligand. Interestingly, we observed a
new set of signals that likely reports on the closed conformation of loop 1, as F23 is one of the
residues that displays a novel conformation upon PrFAR binding (Figure 7, circles). This new
set of signals thus reports on the formation of the closed state of loop1 in the presence of the
ligand analogue. This stable set of signals does not appear in the HisF-G20P and HisF-F23A
variants, proving that the closed conformation is not stably adopted in those cases. This agrees
well with simulation data presented in Figure 5.
Figure 7: ProFAR binding induces a conformational change of loop1 only in wt -HisF and HisF-
F38A. NMR titration experiments recorded in 1H-15N TROSY spectra showing apo HisF (blue) and HisF
in the presence of saturating amounts of ProFAR (red). The large CSP of F23 upon ProFAR binding is
shown by a black arrow. The position of several signals with large CSPs is indicated by black circles.
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Large chemical shift perturbations associated with a substantial conformational change are only
observed in the spectra of wt-HisF and HisF-F38A.
Our combined NMR and stopped flow measurements thus are indicative of a two-step binding
mechanism in the wt-HisF protein, in which the ligand first interacts with the open or detached
conformations of HisF after which loop1 closes to facilitate catalysis (Scheme 1, top).
Scheme 1. Binding of PrFAR to wt-HisF and loop1 variants: Induced fit model versus two-state model
To obtain insights into the rates that are associated with this two-step binding process we
fitted the stopped-flow experiments that were performed under pseudo -first order conditions
for HisF-CouA (excess of HisF-CouA over PrFAR) to the induced-fit model in Scheme 1. These
hyperbolic fits allowed for the determination of the KD1 (= k-1/k1), kconf and k-conf for wt-HisF and
HisF-F38A (Table S3). This shows that the equilibrium of the conformational change is on the
closed side and that a stable closed conformation is thus efficiently formed which subsequently
facilitates efficient substrate turnover. In contrast, PrFAR binding kinetics for the loop1 variants
HisF-F23A and HisF-G20P are compatible with a simple one -step binding reaction (Scheme
1, bottom). The k1 and k-1 values shown in Table S3 result from the slope and intercept with
the y-axis of a linear fit (Figure S6F).
In summary, the NMR and stopped flow experiments, as well as molecular dynamics
simulations, establish that substrate binding to HisF occurs via an induced fit mechanism for
wt-HisF and for the HisF-F38A variant. The HisF-G20P and HisF-F23A variants on the other
hand interact with the substrate via a one step binding mechanism as loop1 is, in those cases,
unable to close properly over the substrate. Interestingly, these variants still interact efficiently
with PrFAR, indicating that loop 1 does not contribu te considerably to the binding energy of
the substrate.
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Product release from wt-HisF and HisF-F38A is more complex than for HisF-F23A and
HisF-G20P
Next, we aimed to obtain insights into the release of the AICAR and ImGP products.
Equilibrium titration measurements showed that both ligands, AICAR and ImGP, can bind
independently to wt -HisF and all loop1 variants, causing a decrease of CouA fluorescence
(Figure 6 ). Exclusively for wt -HisF and HisF -F38A, we noted a significantly higher
fluorescence change when the ternary complex was formed than when the binary complexes
were formed (Table S2), combined with an increase in apparent binding affinity upon formation
of the ternary complex (Table S1). This suggests that the interaction of either product (ImGP
or AIRCAR) does not result in a conformational change in the enzyme, whereas the interaction
with both products at the same time does result in the closing of loop1.
To obtain the rates that are associated with product release from wt-HisF and the loop1
variants we made use of stopped-flow measurements. Representative time traces for wt-HisF
are shown in Figure S7A, the time traces for HisF-F38A resemble those of wt-HisF (data not
shown). As the transient kinetic measurements show, formation of the binary HisF*AICAR and
HisF*ImGP complexes is completed within the dead time of the stopped flow device. Based
on the used enzyme and substrate concentrations and an instrument dead -time of ~2.0 ms,
an observed rate constant kobs of greater than 1000 s-1 is required to obscure all evidence of
association, suggesting that association rate constants for binary complex formation must be
≥ 106 M-1 s-1. In contrast, when monitoring the formation of the ternary complex, fluorescence
changes with rate constants kobs in the range of 50 s-1 were observed. This is visible from the
exponential fluorescence decrease in the stopped -flow transients when the free enzyme
interacts with a mixture of both ligands or when the preformed binary complexes are mixed
with the second ligand (Figure S7A: HisF + ImGP/AICAR, HisF*ImGP + AICAR, HisF*AICAR
+ ImGP). These data thus agree with the equilibrium titrations ( Figure 6 ) that revealed a
synergistic effect when AICAR plus Im GP bind to the enzyme and with the notion that the
interaction with both ligands is associated with a conformational change in the enzyme. In
contrast, in the case of the loop variants F23A and G20P, both the binary and ternary
complexes were formed within the instrument dead -time in stopped -flow measurements
(Figure S7B), which confirms that interaction with both ligands does not lead to loop1 closure
in these variants.
To obtain rate constants for association and dissociation kinetics of the reaction products
AICAR and ImGP a dataset of 16 time traces was recorded by mixing excess of the ligand with
limiting concentrations of HisF CouA or the binary complexes (HisFCouA*I mGP and His
CouA*AICAR). A kinetic model describing ImGP/AICAR binding to HisF (Figure S7C) includes
association and dissociation of the two ligands to the apo enzyme and to the respective binary
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complexes ( k1 and k-1 for ImGP binding as well as k2 and k-2 for AICAR binding) and a
conformational change (the closing of loop 1) to stabilize the ternary complex.
The stopped-flow datasets for wt -HisF (Figure S8) and variant HisF -F38A (Figure S9)
were subjected to a global fitting analysis according to this kinetic model. The curves resulting
from global fitting analysis are indicated by dashed lines. The determined values for the rate
constants are summarized in Table S4. The rate constants obtained for the HisF-F38A variant
in the global fitting analysis resemble those for wt -HisF. Importantly, the KD values for the
binding reactions that were calculated from the global fitting parameters roughly match the KD
values obtained in equilibrium titrations (cf. Table S1 and Table S4). It should be emphasised
that the binding model is a minimal model that accounts for key features of the experimental
data. It could well be that the rate constants for binding of AICAR and ImGP to apo HisF and
the HisF*ImGP/HisF*AICAR complex, respectiv ely, differ. However, this cannot be better
resolved with the stopped-flow datasets, as the binary enzyme-ligand complexes form within
the dead time of the stopped-flow instrument. Importantly, the rates for the loop opening (k-conf)
are higher for the ImGP:AICAR complex than for the PrFAR complex, which indicates that
loop1 opens after the reaction to allow for product release.
The motions of loop1 are not rate limiting in the kinetic mechanism of HisF
To discern which step in the catalytic mechanism is rate -determining for wt -HisF and HisF -
G20P, HisF-F23A, and HisF-F38A, turnover kinetics under multiple turnover conditions were
compared with turnover rates obtained with single turnover conditions. In the multiple turnover
mode HisF was mixed with an excess of the substrate PrFAR and the turnover of PrFAR was
monitored based on the decrease of absorption at 300 nm. Catalytic turnover of PrFAR by
HisF occurs only in the presence of the second substrate ammonia. Therefore, we compared
turnover traces in the presence of ammonia with control traces obtained in the absence of
ammonia to discriminate absorption changes accompanying PrFAR turnover from signals
stemming from binding or mixing reactions. For the re action of wt -HisF a representative
multiple turnover trace and the associated control trace are shown in Figure 8A . The
corresponding data for the HisF variants are shown in Figure S10A (HisF-F38A), Figure S11A
(HisF-F23A), and Figure S12A (HisF-G20P).
The time traces obtained under multiple turnover conditions showed a linear steady -state
phase that is preceded by an exponential burst phase. The burst phase was observed also in
the control curve in absence of ammonia. We attribute this burst phase to a mixing artifact of
the stopped-flow instrument and this phase was not analyzed any further. Turnover velocities
were deduced from a linear fit of the steady-state phase and were plotted as a function of the
PrFAR concentration to obtain the kcat and KMPrFAR values for wt-HisF (Figure 8B) and HisF-
F38A, HisF-F23A, and HisF-G20P (Figures S10B – S12B).
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For measurements under single -turnover conditions the substrate PrFAR was saturated
with enzyme so that all PrFAR molecules participate in the single turnover. The rate of turnover
rate in that case is unaffected by product release and can be determined by fitting the change
in the fluorescence over time to a single-exponential function. A representative single-turnover
transient for wt-HisF is shown in Figure 8C. The corresponding data for the HisF variants are
shown in Figure S1 0C (HisF-F38A), Figure S1 1C (HisF-F23A), and Figure S1 2C (HisF-
G20P). Single-turnover rates kobs determined from these exponential fits were independent of
the applied PrFAR concentrations, both for wt-HisF (Figure 8D) and the variants HisF-F38A,
HisF-F23A, and HisF-G20P (Figure S10D- S12D). The kinetic constants determined for the
multiple and single turnover measurements are summarized in Table S5.
Figure 8: Multiple - and single -turnover kinetics of the wt -HisF reaction. (A) Representative
transient monitoring PrFAR conversion in multiple turnover mode at 25°C after mixing 0.1 µM HisF with
10.0 µM PrFAR (final concentrations) in the presence of 100 mM ammonium acetate (turnover curve,
blue line). A linear approximation of the steady-state phase (dashed line) yielded a turnover velocity of
v = 0.192 µM s -1. The control curve (light blue line) shows the progress of the reaction in absence of
ammonium acetate. (B) Plot of the turnover velocity v vs. the respective PrFAR concentration in multiple
turnover experiments. kcat and KMPrFAR-values were obtained by fitting to the Michaelis-Menten equation.
(C) Representative transient monitoring PrFAR conversion in single turnover mode after mixing an
excess of HisF (20 µM) with 10 µM PrFAR in the presence of 100 mM ammonium acetate (turnover
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curve, red line). The turnover curve was fit with a single exponential decay function (dashed line, 𝑦 =
𝑎 ∗ 𝑒!"!"#∗$ + 𝑐). The control curve (orange line) shows the progress of the reaction in the absence of
ammonium acetate. (D) Plot of the turnover rates, kobs, observed under single turnover conditions, vs.
the respective PrFAR concentration. kcat-, KM- and kobs-values are summarized in Table S5.
In summary, turnover rate measurements confirm that variant HisF-F38A is catalytically as
active as wt-HisF, whereas the activities of the two loop1 variants HisF-F23A and HisF-G20P
are significantly reduced. This deterioration of catalytic activity manifests mainly in kcat values
and single -turnover rates, which are reduced by three orders of magnitude, but is also
expressed in a 2 to 5 -fold increase of the KM values. Remarkably, rate constants obtained in
multiple and single turnover measurements have the same order of magnitude, implying that
product release and associated conformational changes are not rate determining in the
catalytic mechanism. Hence, it is concluded that the chemical step is rate -determining for
catalysis by HisF. This is in contrast to other enzymes in this pathway, such as HisA and PriA,
where loop motion is likely rate determining.32
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