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Báo cáo khoa học: Spectroscopic investigation of the reaction mechanism of CopB-B, the catalytic fragment from an archaeal thermophilic ATP-driven heavy metal transporter potx

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Starting from the E1 state, with high binding affinity for the substrates ions and nucleotides on one side of the membrane, the terminal c-phosphate group of ATP is transiently transferre

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CopB-B, the catalytic fragment from an archaeal

thermophilic ATP-driven heavy metal transporter

Christian Vo¨llmecke, Carsten Ko¨tting, Klaus Gerwert and Mathias Lu¨bben

Lehrstuhl fu¨r Biophysik, Ruhr-Universita¨t Bochum, Germany

Introduction

The biological role of P-type ATPases is ATP-driven

transport of ions against their concentration gradients

along membranes They form a heterogeneous

super-family, which has been divided into several categories

according to sequence similarity and substrate

specific-ity [1] Among these, the Ca- and Na⁄ K-ATPases

belong to the well-studied class II enzymes Another

large group (class Ib) comprises the so-called

CPX-ATPases, which are responsible for the import or

export of soft metals, such as copper, zinc, silver, lead,

cobalt or cadmium

CPX-ATPases are evolutionarily related and have a

common architecture, consisting of a hydrophobic part

with a predicted eight transmembrane helices, in which

the central ion binding site resides Their peripheral part is extensively hydrophilic and contains several structural and functional modules, such as nucleotide binding (N), phosphorylation (P), actuator (A) and heavy metal binding (HMA) domains

During the catalytic cycle, P-type ATPases, also called E1E2-ATPases, undergo ordered large-scale domain movements, in which ion translocation is coupled to the energy released from ATP hydrolysis Starting from the E1 state, with high binding affinity for the substrates (ions and nucleotides) on one side

of the membrane, the terminal c-phosphate group of ATP is transiently transferred to a conserved aspartic acid, forming a covalently bound aspartyl-phosphate

Keywords

fluorescence spectroscopy;

Fourier-transform infrared spectroscopy;

heavy metal translocation; P-type ATPase;

reaction mechanism

Correspondence

M Lu¨bben, Lehrstuhl fu¨r Biophysik,

Ruhr-Universita¨t Bochum, Universita¨tsstr.

150, D-44780 Bochum, Germany

Fax: +49 234 32 14626

Tel: +49 234 32 24465

E-mail: luebben@bph.rub.de

(Received 14 May 2009, revised 24 July

2009, accepted 21 August 2009)

doi:10.1111/j.1742-4658.2009.07320.x

The mechanism of ATP hydrolysis of a shortened variant of the heavy metal-translocating P-type ATPase CopB of Sulfolobus solfataricus was studied The catalytic fragment, named CopB-B, comprises the nucleotide binding and phosphorylation domains We demonstrated stoichiometric high-affinity binding of one nucleotide to the protein (Kdiss 1–20 lm) Mg

is not necessary for nucleotide association but is essential for the phospha-tase activity Binding and hydrolysis of ATP released photolytically from the caged precursor nitrophenylethyl-ATP was measured at 30C by infra-red spectroscopy, demonstrating that phosphate groups are not involved in nucleotide binding The hydrolytic kinetics was biphasic, and provides evidence for at least one reaction intermediate Modelling of the forward reaction gave rise to three kinetic states connected by two intrinsic rate constants The lower kinetic constant (k1= 4.7· 10)3s)1at 30C) repre-sents the first and rate-limiting reaction, probably reflecting the transition between the open and closed conformations of the domain pair The subse-quent step has a faster rate (k2= 17· 10)3s)1 at 30C), leading to prod-uct formation Although the latter appears to be a single step, it probably comprises several reactions with presently unresolved intermediates Based

on these data, we suggest a model of the hydrolytic mechanism

Abbreviations

cgATP, caged ATP; mant-ATP, 3¢-N-methylanthraniloyl-ATP; AMPPNP, adenosine 5’(b,c-imido)triphosphate.

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intermediate The phosphorylated E1 state switches

to the phosphorylated E2 state with low affinity for

the substrate ion, which is released to the other side

of the membrane after hydrolysis of the phosphoryl

bond Extensive information about the catalytic

mechanism has been obtained from investigations of

various P-type ATPases [2–5] Many details on the

molecular function and structural models of ground

state and various intermediate states have been

obtained for Ca-ATPase [6], which is regarded as

virtually paradigmatic for the P-type ATPases

Ca-ATPase and Na⁄ K-ATPase have been extensively

investigated by time-resolved FTIR absorbance

differ-ence spectroscopy using various nucleotides and

nucleo-tide analogues [7–13] These studies have suffered from

the fact that the described mammalian proteins could

only be purified from native tissue material The

holo-proteins were difficult to express in Escherichia coli,

which precluded the use of site-directed mutant proteins

or group-specific isotopically labelled proteins for

spec-tral comparisons, which are crucial for assignment of

protein-associated absorbance difference bands

Bacterial CPX-ATPases consist of a single subunit

and can be readily expressed in the heterologous host

Escherichia coli Proteins of this subclass are therefore

suited for site-directed mutagenesis, and would be ideal

candidates for the study of molecular reaction

mecha-nisms However, the 3D structure, which would be

enormously helpful in understanding the molecular

mechanism of CPX-ATPase, is unknown Previously,

various attempts at comparative modelling have created

a structural model of the holoenzyme [14–16] Using

‘divide and conquer’ strategies, the partial 3D structures

of various modules have been determined, such as the

HMA domain of the CPX-ATPases of Listeria

mono-cytogenesand Bacillus subtilis, the N⁄ P and A domains

of Archaeoglobus fulgidus CopA and the N⁄ P domains

of Sulfolobus solfataricus CopB [17–21] In order to

study the reaction mechanism of the ATPase, we

explored here whether a truncated variant of CopB could

act as model for the holoenzyme Therefore, the soluble

catalytic fragment CopB-B, comprising the hydrophilic

N⁄ P domains of CopB from Sulfolobus solfataricus

(Fig 1) was probed The activities of the catalytic

fragment were investigated using enzymological,

fluores-cence [22] and infrared spectroscopy [23] methods

Results

Nucleotide binding to CopB-B

The catalytic fragment N⁄ P, also called CopB-B,

con-sists of the nucleotide binding and phosphorylation

domains of the thermophilic CPX-ATPase CopB from

S solfataricus It was expressed in E coli, crystallized

in a nucleotide-free state, and its structure was deter-mined [21] (see Fig 1) The domains are connected by hinge peptides, which allow substantial flexibility of both domains relative to each other The domains appear to be in a so-called closed orientation, into which the substrate nucleotide, ATP, has been modelled by superposition on the nucleotide-bound structure of Ca-ATPase (Fig 1) The purine moiety fits into a cleft of the nucleotide-binding domain, whereas

Fig 1 3D structural model of the catalytic fragment CopB-B of the heavy metal-translocating CPX-ATPase CopB from Sulfolobus solfa-taricus (PDB code 2IYE) The protein is displayed in half-transparent molecular surface representation, and the conserved phosphoryl-atable Asp416 is shown The adenine nucleotide shown was modelled after structural superposition with the ADP ⁄ AlF 3 -bound structure of Ca-ATPase (PDB code 1WPE).

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the phosphate groups are located in the vicinity of the

phosphorylation domain It should be taken into

account that our model of the nucleotide-bound state

of CopB-B is relatively crude with respect to the

phos-phate region, and should not be interpreted as

assign-ing possible protein interaction sites to functional

groups of the substrate [21]

The binding interaction of CopB-B with various

adenine nucleotides under stoichiometric conditions

was qualitatively verified by gel filtration of the

nucleo-tide⁄ protein complex and subsequent analysis of the

nucleotides of the collected fractions using

high-perfor-mance liquid chromatography on a reverse-phase

column (see Appendix S1) Equilibrium binding of

nucleotides was quantitatively investigated using the

fluorescent analogue 3¢-N-methylanthraniloyl-ATP

(mant-ATP) (Fig 2) Binding to the protein at

saturat-ing nucleotide concentrations resulted in a 4.5-fold

increase of emission intensity, demonstrating that the

fluorophore becomes positioned in a location that is

less exposed to quenching molecules In addition, the

emission peak shifts from 444 to 434 nm, indicating

that, upon binding, the fluorescent substituent moves

from the hydrophilic solvent into the more

hydropho-bic protein environment (Fig 2A) To assess the

speci-ficity of binding, we displaced the bound mant-ATP

by addition of excess ATP The kinetic dissociation of

the mant-ATP⁄ protein complex appears to be

rela-tively rapid, as the process could not be resolved

within the manual mixing time This reversible ligand

competition shows that the nucleotide portion of the

analogue is responsible for the specific interaction with

the protein

A titration of the nucleotide binding site under

stoi-chiometric conditions (i.e when the molar

concentra-tions of mant-ATP and protein have values much

greater than Kdiss) resulted in a linear increase of

fluo-rescence with ligand addition up to the saturation

point, and above it in constant fluorescence (data not

shown) Extrapolating the lines to their intercept gave a

binding stoichiometry of one nucleotide per CopB-B fragment

For determination of the binding constant Kdiss, the conditions were adjusted such that the concentrations

of mant-ATP and protein were of the same order as the expected Kdiss The hyperbolically shaped titration

A

B

C

Fig 2 Equilibrium binding of CopB-B with nucleotides (A)

Fluores-cence spectra of 0.5 l M mant-ATP in 5 m M Na ⁄ Mes buffer, pH

6.2, at room temperature in the absence (dashed lines) or presence

(continuous lines) of CopB-B in large stoichiometric excess (15 l M ).

(B) Fluorescence titration of 0.5 l M mant-ATP with CopB-B The

fluorescence at emission wavelength 434 nm is given in arbitrary

units; [Et] = total concentration of CopB-B (C) Determination of

ligand dissociation constants from competitive titrations of 0.5 l M

CopB-B with mant-ATP in the presence of the indicated total

con-centrations ([L0]) of ATP (squares), ADP (circles) and AMP

(trian-gles) for determination of the apparent Kdissapp Data were analyzed

according to Eqn (4) The bars indicate K app

diss errors from individual fits of titration curves obtained at fixed competitor concentrations.

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curve under experimental condition 1 described in the

Experimental procedures (mant-ATP held constant) is

shown in Fig 2B A non-linear regression fit of the

measured data results in a binding constant of 1 lm

according to Eqn (1) The same results were obtained

when titrations were performed under experimental

condition 2 (protein held constant) Nucleotide binding

was highly sensitive to the salt concentration, with the

Kdiss increasing to 40 lm at 100 mm NaCl or

(NH4)2SO4 Notably, binding does not require Mg2+;

the affinity is reduced by a factor of 10 in the presence

of 1 mm MgCl2(Table 1)

The binding specificity of the protein to mant-ATP

can be demonstrated by its displacement by other

nucleotides that are added in slight excess to the

complex It is clear from the displacement of bound

mant-ATP by ATP and related compounds that these

nucleotides interact with the same protein binding

site Ligand competition could thus be exploited for

determination of binding constants of non-fluorescent

nucleotides According to Eqn (4), the apparent

affin-ity Kdissapp of CopB-B for mant-ATP is significantly

increased with higher concentrations of competitor

nucleotide Based on a series of fluorescence titrations

of mant-ATP to CopB-B in the presence of various

competitor concentrations [L0], the binding constant of

the nucleotide can be determined from the slope of

the linear plot of the apparent binding constants Kdissapp

and [L0] With the ligand ATP, a binding constant

Kdisslig of 10 lm was obtained (Fig 2C) The

non-hydro-lysable analogue adenosine 5¢(b,c-imido)triphosphate

(AMPPNP) had binding properties comparable to

those of ATP (Table 1) Structural modification of the

purine moiety had no significant effect, as ATP and

GTP showed affinities in the same order of magnitude

On the other hand, ADP, the product of the ATPase reaction, bound to CopB-B with approximately half of the affinity of ATP AMP had a comparable Kdisslig of approximately 30 lm (Table 1), which indicates that the b- and c-phosphate groups are less important for the binding process than the base⁄ sugar part A remarkable observation is the binding of caged ATP (cgATP) with an affinity similar to that of ATP (Table 1), which was verified independently by HPLC (see Fig S1)

Catalytic activity During catalytic activity, the c-phosphate of ATP is transiently transferred onto the strictly conserved aspartic acid located in the phosphorylation domain, which is Asp416 in CopB-B [21] In the P-type ATPase holoprotein, the A domain comes into contact with the

N⁄ P domain pair, promoting the hydrolysis reaction

by release of inorganic phosphate from the phosphory-lated intermediate state [5] Formation of the phos-phorylated intermediate of CopB-B with the substrate ATP has been shown previously [24], as well as its hydrolytic activity with the artificial substrate p-nitro-phenyl phosphate, even though the A domain is absent

in this construct This is probably due to thermal activation of the phosphatase reaction The catalytic activity using the native substrate Mg-ATP gave approximately five times higher rates, amounting

to 50–70 nmol (mgÆmin))1 Variation of substrate concentration revealed a simple hyperbolic Michaelis– Menten-type dependence and a KM of 1 mm, which reflects relatively poor kinetic substrate affinity compared with the thermodynamic ligand association constant Kdisslig of ATP (Fig 3A) Nevertheless, these relationships are consistent because high substrate con-centrations are needed to overcome the high-affinity binding of the product ADP (Table 1) under kinetic steady-state conditions No production of inorganic phosphate was observed in the absence of Mg2+, which indicates that Mg-ATP is the substrate of CopB-B Furthermore, the ATPase activity increased in the temperature interval between 20–70C (Fig 3B) At higher incubation temperature, the thermophilic protein starts to denature The protein is an active hydrolase under single turnover conditions at room temperature

as demonstrated for stoichiometric loading with Mg-ATP by HPLC analysis (data not shown) Notably, the catalytic fragment is still active at a temperature of

30C, which is important with regard to our approach

to investigate the molecular reaction mechanism using time-resolved FTIR spectroscopy (see below)

Table 1 Binding of nucleotides to the catalytic fragments of

CPX-ATPase CopB The interaction is quantified from apparent binding

constants obtained by competitive binding titration of mant-ATP in

the presence of various concentrations of nucleotides Unless

indicated otherwise, Mg 2+ was omitted to prevent phosphatase

activity.

Nucleotide Binding constant Kdisslig (l M ) a

mant-ATP b ⁄ 1 m M MgCl2 10.0

a According to Eqn (4) b For mant-ATP in the absence of

competi-tor, the value for Kdissis given.

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Molecular interaction of ATP with CopB-B

Transient reactions were routinely observed using

rapid mixing techniques However, these are difficult

to perform in the case of time-resolved FTIR

spectros-copy The use of cuvettes with an optical path length

of less than 10 lm is imperative due to the high

absor-bance of water in the infrared region Under these

cir-cumstances, the reaction mechanism of the ATPase

can best be studied by release of ATP from the caged

precursor compound cgATP by photochemical

activa-tion according to the following reacactiva-tion scheme:

where kph represents the kinetic constant describing the fast photolytic cleavage of the caged compound It

is clear from equilibrium binding of cgATP (Table 1) that the CopB-BÆcgATP complex has already formed before photolysis To this end, samples were prepared

in special FTIR cuvettes with high concentrations of CopB-B and the Mg2+ complex of cgATP The com-ponents were present at a 1 : 1 ratio in order to pre-vent more than a single catalytic turnover Upon light activation for an integrated duration of 0.12 s, the genuine substrate is released

In order to clearly differentiate the post-flash IR absorbance signals into the photochemical processes of ATP release [25] and the subsequent hydrolytic protein reactions, the photochemical non-enzymatic process, which is strongly dependent on temperature and the

pH of the medium, must be the fastest reaction step The rapid appearance of positive absorbance changes

at 1123 cm)1 generated from free cgATP (Fig 4A, continuous line) and from cgATP in the presence of CopB-B (Fig 4A, dotted line) within the phosphate region of the infrared spectrum is indicative of product formation This band was assigned to the symmetric stretching vibration of the c-PO3 )group of ATP [25], thus providing information on the photochemical release rate of ATP from its caged precursor molecule The time course of the difference band corresponds to rates of 4 and 7 s)1 in the presence or absence of CopB-B, respectively, which demonstrates that the release of ATP is much faster than all subsequent partial reactions (see below), and, furthermore, gives a constant reference line for the pre-photolytic state of CopB-BÆATP after less than 2 s (Fig 4A)

Static photolysis spectrum and phosphate band assignment

The absorbance difference bands that are directly visi-ble in the spectra after photolysis of cgATP and those resolved by global fit analysis (see below) were assigned using substrate isotopologues [26] The IR difference spectrum recorded directly after photo-release indicates the binding state of the pre-existing CopB-BÆATP com-plex before the start of hydrolysis (Fig 4B) Negative difference bands at 1525 and 1347 cm)1 refer to the symmetric and anti-symmetric vibrations of the NO2 group in cgATP identified previously [25] For compari-son and further band assignment, spectra were run under identical conditions with ATP isotopically labelled at specific positions, i.e by chemical substitu-tion of 16O for 18O in the phosphate groups The increase in weight results in higher reduced masses of the molecular oscillators and therefore lowering of the

A

B

Fig 3 Catalytic properties of CopB-B (A) Substrate kinetics of

10 l M CopB-B with Mg-ATP at 70 C (B) Temperature dependence

of 10 l M CopB-B at an Mg-ATP concentration of 5 m M The pH of

the Na ⁄ Mes incubation medium at various temperatures was kept

constant between 5.9 and 6.2.

Scheme 1.

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vibrational frequencies As a typical example, Fig 4C

shows the photolysis spectrum of CopB-B with ATP

and c-18O4-ATP, respectively The positive band at

1137 cm)1 observed in the 16O compound is

down-shifted to 1089 cm)1 in the c-18O4-labelled ATP, and

this band can therefore be assigned to the

anti-symmet-ric stretching vibration of the c-phosphate group [ma (c-PO3 ))] Minor deviations of the observed band frequencies from tabulated values could relate to the

pH dependence of phosphate resonances and their shifts induced by formation of Mg complexes [25,27] Further band assignments are summarized in Table 2 (corresponding spectra not shown) It is worth noting that, in the CopB-B-bound state, the phosphate vibrations are coupled, as seen for example in the absorbance band at 1123 cm)1, which is shifted to

1101 cm)1 irrespective of placement of the18O label in the b or a group Strong phosphate coupling is other-wise known only for nucleotides in free aqueous solu-tion [26] In sharp contrast to CopB-B, phosphate coupling is abolished in the case of the GTP-binding protein Ras, in which phosphate absorbances are significantly shifted with respect to the non-bound state [26] and coupling between the a and b groups is removed The close similarity of IR difference spectra

of nucleotides in the presence and absence of CopB-B leads to the conclusion that the phosphate groups of ATP apparently do not contribute significantly to the formation of the nucleotide–protein complex; instead they are positioned in a hydrophilic environment or even remain solvent-exposed

Dynamic interaction of ATP with CopB-B:

time-resolved hydrolysis spectra revealing a reaction intermediate

After rapid release of the substrate ATP, its hydrolysis was observed to occur at comparatively low rates As

a control, the time course of the absorbance changes after photo-release was recorded in the spectral range from 1000–1800 cm)1 in the absence of protein, which demonstrates insignificant spectral contributions from cgATP and its photolysis alone (for details, see Fig S2) Upon elimination of the data related to the

A

B

C

Fig 4 Investigation of the ATPase reaction by FTIR spectroscopy (A) Time course of ATP photo-release from cgATP The absorbance changes of the symmetric coupled a,b-phosphate band of ATP at

1123 cm)1 (cgATP photolysed in presence of CopB-B, continuous line; cgATP photolysed alone, dotted line) were recorded by rapid-scan FTIR spectroscopy (B) Photolysis spectra of cgATP in the presence (continuous line) and absence of CopB-B (dotted line) The difference spectrum was obtained after 2 s, when ATP was fully released (C) Principle of band assignment of phosphate absor-bance difference bands in the photolysis spectrum by means of

18 O-labelled phosphates (dotted line) The reference spectrum (continuous line) was obtained with unlabelled ATP The absor-bance difference band (hatched upwards) is downshifted to another position (hatched downwards) in the spectrum obtained using c-18O 4 -labelled ATP under otherwise identical conditions.

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extremely fast initial photolytic phase (Fig 4A), the

relatively slow hydrolytic reaction rates were

kinetical-ly anakinetical-lysed by global fitting We were able to simulate

the spectral absorbance changes by multi-exponential

regression analysis with two rate constants k1app and

k2app Thus, to describe the overall hydrolysis reaction,

we derived a tentative working model displayed in

Scheme 2, consisting of the pre-hydrolytic initial state

(CopB-BÆATP), an intermediate (I) and a final state

(CopB-BÆADP):

In addition to the quickly formed so-called

photoly-sis spectrum ‘CopB-BÆATP–CopB-BÆcgATP’ (Fig 4B),

the consecutive reaction of the three protein states

connected by the two apparent rate constants is

repre-sented by two amplitude difference spectra )a1 and

)a2for the two rate constants k1app(Fig 5A, top) and

k2app (Fig 5A, bottom) Under the applied reaction

conditions, the first amplitude spectrum (k1app) could

be resolved with a rate constant of 1.9· 10)2s)1

(Fig 5A, top) and the second with a rate constant

(k2app) of 5· 10)3s)1(Fig 5A, bottom)

Kinetic modelling of CopB-B’s ATPase reaction

If the apparent rate constants k1app and k2app derived

from the global fitting differ only by a factor of four,

as in our case (Table 3), analysis of the spectral com-ponents of the amplitude spectra )a1 and )a2

(Fig 5A) becomes complicated due to mixing of states

In such a case, apparent and intrinsic rate constants often deviate drastically from each other For deter-mination of intrinsic rate constants for the ATP hydro-lysis, we applied the kinetic modelling program KinTek Global Kinetic Explorer [28] using the fol-lowing model (Scheme 3) with intrinsic rate constants

k1, k)1, k2and k)2:

In order to determine the intrinsic rate constants, we assumed that the concentration changes of CopB-BÆATP, the intermediate I and Piare proportional to the absorption changes at 1255 cm)1 (vas a-b-ATP band),

1338 cm)1 (unidentified protein side chain band) and

1078 cm)1 (inorganic phosphate band), respectively In addition, we normalized both the starting reactant (educt) absorbance at 1255 cm)1and the product absor-bance at 1078 cm)1, so that c0 (CopB-BÆATP) = c¥ (Pi) = 1 and c¥(CopB-BÆATP) = c0 (Pi) = 0 Due to the unknown absorption coefficient of the intermediate

I, we arbitrarily averaged both normalization factors for CopB-BÆATP and Pito obtain a reference for its relative concentration Based on these assumptions, we consid-ered models 1 and 2 described below

Model 1 is a simulation based on free parameter optimisation of the program, and yields k1= 4.7·

10)3s)1, k)1= 3.0· 10)4s)1, k2= 1.7· 10)2s)1and

Table 2 Assignment of phosphate vibration detected in the Mg-adenine nucleotide complexes of CopB-B by means of 18 O-labelled ATP iso-topologues.

Spectrum according

to global fit v (cm)1) Band assignment

Band position after shift upon addition of isotopolog

Deflection of the difference band d

18 O4-c (cm)1) 18 O3-b (cm)1) 18 O2-a (cm)1)

a

Assignment to more than one phosphate group indicates strong vibrational coupling [27].bsp., superposed Absorbance difference bands disappear upon isotopic labelling, but shifts are not observed due to complex band superposition c Amplitude spectra corresponding to the apparent rate constants k1app and k2app due to global fitting d u = upward, d = downward.

Scheme 2.

Scheme 3.

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k)2=1.0· 10)4s)1(Table 3) The corresponding con-centration profiles of the three components (Fig 6A) agree well with our normalized data (squares), indicat-ing reasonable selection of scalindicat-ing factors The main fea-tures of this kinetic model are that k2> k1(k2 k1app;

k1 k2app), and that back reactions are negligible The faster decline of the intermediate compared to its forma-tion leads to only small concentraforma-tions of intermediate I during the reaction The maximum concentration of I is approximately one-eighth of that of c0 (CopB-BÆATP) This is similar to the relatively small absorbance change

at 1338 cm)1compared to 1078 or 1255 cm)1, and thus

in line with our measurements

In model 2, parameters were fixed as suggested by global fitting, namely k1> k2 and k1 = k1app, and

k2= k2app and k)1= k)2= 0 Given these assump-tions, Fig 6B shows that the measured normalized absorbance at 1255 cm)1, indicative of the time course

of educt concentration, clearly deviates from its calcu-lated concentration profile Moreover, this simulation yields notably higher concentrations of the intermedi-ate than the former model

To further check the rationality and stability of our model assumptions, we varied the extinction coefficient

of the intermediate I for both models 1 and 2 (see Dis-cussion and Fig S3) In neither case did the simulated curves give better fits to the measured data than the ones displayed in Fig 6A Of even greater significance than the extinction coefficient of the intermediate I are the concentration profiles of educt and product, which both match optimally with curve fit 1 In summary, fit

1, based on program-chosen intrinsic constants, maps the time course of the reactant concentrations much better than fit 2, based on fixed constants; fit 1 therefore supports a credible model The data from model 1 were thus used to calculate the relative contributions of the states to the amplitude spectra )a1 and )a2 of the global fit as detailed in Appendix S1 The result of this calculation is that the bands facing upwards in )a1

(Fig 5A, top) derive from the intermediate state, and

A

B

Fig 5 FTIR spectroscopic measurement of the ATPase reaction as

performed by CopB-B, initiated by flash-initiated substrate liberation

of ATP from cgATP Rapid scan spectra recorded with a repetition

time of 185 ms (using double-sided forward–backward mode) fitted

to two rate constants by global fit analysis, k1app = 1.9 · 10)2s)1

and k 2app= 5 · 10)3s)1, starting from 2 s after the flash The band

labelled X is an artefact that also occurs in the sample without

pro-tein (A) Amplitude spectra corresponding to the rate k1app ( )a 1 , top)

and the rate k 2app ( )a 2 , bottom) (B) Band assignment verifying

phosphate production in the k 2apptransition by comparison of

ampli-tude spectra recorded with 16 O (continuous line) and 18 O (dotted

line) ATP isotopologues (top) and after double difference calculation

(16O–18O difference spectra) (bottom) The hatched zones indicate

the loss of c-ATP in the precursor state and the formation of

inorganic phosphate at the final stage of the phosphatase reaction.

Table 3 Kinetic constants obtained by various theoretical methods

of examination.

Kinetic stepa Rate constantb(s)1)

a

The steps are defined according to Schemes 2 or 3.bRate con-stants were calculated by data approximation via global fit [apparent rate constants (kiapp )] or via kinetic modelling (model 1; ki).

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the bands facing downwards derive from the final ADP

state The intensities are 38% compared to pure states

The bands facing downwards in )a2 derive from both

the intermediate state (38%) and the initial ATP state,

and the bands facing upwards in )a2 derive from the

final ADP state

The intermediate state during ATP hydrolysis

As the absorbances of the intermediate are facing

upwards in )a1 and downwards in )a2 (Fig 5A), the

appearance and disappearance of a band at 1338 cm)1 may be regarded as a marker of this intermediate It represents an unknown absorbing group of the protein, because absorbances in this region are clearly distinct from the phosphate vibrations Furthermore, the amplitude spectra displayed in Fig 5A indicate signifi-cant changes in the broad amide I band centered at approximately 1650 cm)1, and especially pronounced

at 1676 cm)1, and in the amide II band position at

1546 cm)1 This is not unexpected, as it is known that P-type ATPases undergo remarkable structural changes during catalysis Another interesting feature is the reproducible occurrence of small positive and nega-tive absorbance difference signals in the carbonyl region of the IR spectra in the region of 1720–

1740 cm)1, seen in both the )a1 and )a2 amplitude spectra (Fig 5A) Signals in this region point to the prevalence of protonated aspartic or glutamic acid side chains either undergoing protonation⁄ deprotonation reactions or conformational reorganizations

End product state of CopB-B-catalysed ATP hydrolysis

As mentioned above, the bands of the end product are the bands facing upwards in )a2 (Fig 5A, bottom) The shift of the positive band from 1078 to 1043 cm)1 upon c-18O-ATP labelling clearly demonstrates the for-mation of free inorganic phosphate in the product state, which becomes obvious in the absorbance differ-ence, and especially in the double difference spectrum (Fig 5B) Further product bands are found at 1220 and 1098 cm)1, which are assigned to the a and b vibrations of the hydrolysis product ADP (Table 2) Isotopic labelling at the c-18O-ATP position shifts the negative ms c-ATP band from 1136 to 1108 cm)1 (Fig 5B, curved arrow) As expected, the negative bands at 1255 and 1136 cm)1 (Fig 5A, bottom) corre-spond well with the positive bands in the photolysis spectrum (Fig 4B) from a-, b- and c-coupled ATP vibrations (Table 2)

Discussion

CopB-B is a suitable model to study ATP hydrolysis of the P-type ATPase CopB

We have measured significant basal ATPase activity of CopB in absence of the heavy metals (M Zoltner &

M Lu¨bben, unpublished observations) Similarly, metal-independent hydrolytic activity has also been observed with the CPX-ATPase CopA of Thermo-toga maritima [29] CopB-B can mimic the effects of

A

B

Fig 6 Time course of computed reactant concentrations after

kinetic modelling of the reaction between CopB-B and ATP The

normalized concentrations of reactants were plotted as fractions of

1 over time (educt CopB-BÆATP, red line; reaction intermediate I,

black line; product inorganic phosphate Pi, blue line) In addition,

the normalized measured absorbances of educt at 1255 cm)1

(CopB-BÆATP), of reaction intermediate at 1338 cm)1(unidentified

protein functional group) and of product at 1078 cm)1 (inorganic

phosphate Pi) are plotted (squares) Simulations were performed

under the two conditions: fit 1, for which intrinsic rate constants

k1, k2, k)1and k)2were optimized using the program KinTek Global

Kinetic Explorer (continuous lines) (A), and fit 2, for which fixed

rate constants k 1 = k 1appand k 2 = k 2app, k)1= k)2= 0 were chosen

(B).

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CopB-ATPase, which are entirely independent of the

translocated heavy metals, as the fragment naturally

carries out ‘uncoupled’ hydrolytic activity Our efforts

demonstrate that spectroscopic methods can be used to

study the substrate binding and catalytic activity of the

hyperthermophilic Sulfolobus enzyme CopB, because it

is easily handled at room temperature The catalytic

fragment CopB-B, consisting of nucleotide-binding

and phosphorylation domains, is the natively folded

‘business end’ of the holoenzyme CopB It is expected

that this fragment, whose 3D structure is known,

behaves similarly to the holoenzyme with respect to

ATP hydrolysis and thus serves as a model of it The

protein is capable of forming an intermediate with

covalently bound inorganic phosphate [24], and has

considerable ATPase activity despite the absence of the

actuator domain (A domain), which is considered to

promote rapid cleavage of the aspartyl phosphate

bond in Ca-ATPase [30] At 30C, the ATP hydrolysis

rate of CopB-B is fairly low, but still allows

observa-tion of the reacobserva-tion with substrate produced from

cgATP under single turnover conditions with a half-life

of approximately 3 min

Nucleotide binding to CopB-B

In order to precisely define the reaction conditions of

the spectroscopically observed CopB-B reaction with

ATP, the interaction of nucleotides with CopB-B was

explored by direct equilibrium binding or competition

assays using the fluorescent nucleotide mant-ATP As

has also been observed with other purine nucleotides,

cgATP has high affinity for CopB-B, which proves

that, within the applied concentration range of the

FTIR experiments ([cgATP]0>> Kdisslig (cgATP)), a

complex between the components has already formed

before photolysis After laser flash photolysis of

cgATP, the substrate ATP is released at the position

of its binding site, so this aspect of complex

associa-tion can be ignored for the kinetic interpretaassocia-tion of

our data

The nucleotide binding spectrum of CopB-B

obtained immediately after photolysis (Fig 4B) shows

a striking similarity to the spectrum of free ATP,

which is in sharp contrast to observations made with

several GTP-binding proteins such as Ras, Ran, Rab,

Rap and Rho, which exhibit vibrational uncoupling of

the phosphate resonances and significant shifts of the

a, b and c absorbance bands, resulting from strong

interactions of phosphate groups with amino acid side

chains lining the nucleotide binding site of the protein

[26,31–34] It is concluded that, in CopB-B, the

phos-phates stay in contact with the solvent, and the tightly

bound ATP becomes immobilized by other molecular parts of the nucleotide, presumably the purine moiety, which apparently protrudes into a binding pocket formed by CopB-B as seen in Fig 1

CopB-B interacts with ATP in a multi-step process

ATP hydrolysis of CopB-B apparently includes two phases These are kinetically resolved by global fit analysis and reflect the formation and decay of a single observable reaction intermediate Given the many intermediates that have been recognized during the reaction mechanism of P-type ATPases [2,35], more than one intermediary state would also be expected to occur during observation of hydrolysis with FTIR spectroscopy For example, there is spectral evidence for protonated carboxyl groups, of which one is expected as a potential phosphate acceptor in P-type ATPases [13], within the absorbance region of 1720–

1740 cm)1 (Fig 5A,B) Spectroscopic signatures of a transiently phosphorylated aspartic acid, as demon-strated earlier for Ca-ATPase [12], could not be resolved in our samples Details on the as yet unre-solved catalytic steps may be disclosed after careful adjustment of reaction conditions by either freezing otherwise invisible intermediates or investigating site-specific mutants

Kinetic process of ATP hydrolysis Kinetic modelling requires theoretical values for cata-lytic events as an input, but delivers a more detailed interpretation of measured data than global fitting Obvious deviations from recorded absorbance data occur, as in fit 2 (Fig 6B), in which the intrinsic rate constants were arbitrarily chosen as equal to the apparent constants In contrast, concentration profiles closely matched the absorbance time courses in the case where the intrinsic constants were adjusted (fit 1, Fig 6A) The educt decrease (CopBÆATP) takes place with the slower intrinsic rate k1, and the product increase (Pi) proceeds with the faster rate constant k2 Therefore, a relatively low concentration of intermedi-ate is seen, as the decay rintermedi-ate k2 of intermediate I is faster than its production rate k1 The slower rate k1 should be associated to the first process after release of ATP, i.e the conformational change of CopB-B leading to the ‘closed conformation’ In this step, the hydrophilic environment of the phosphate groups of ATP is substituted by a specific catalytic environment within a binding pocket of the protein This should induce dramatic absorption changes within the

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