molecules
Review High-Pressure Mechanistic Insight into Bioinorganic NO Chemistry
Łukasz Orzeł 1, Maria Oszajca 1 , Justyna Polaczek 1 , Dominika Por˛ebska 1 , Rudi van Eldik 1,2,* and Grazyna˙ Stochel 1,*
1 Faculty of Chemistry, Jagiellonian University, Gronostajowa 2, 30-387 Kraków, Poland; [email protected] (Ł.O.); [email protected] (M.O.); [email protected] (J.P.); [email protected] (D.P.) 2 Department of Chemistry and Pharmacy, University of Erlangen-Nuremberg, Egerlandstr 1, 91058 Erlangen, Germany * Correspondence: [email protected] (R.v.E.); [email protected] (G.S.); Tel.: +48-66-777-2932 (R.v.E.); +48-12-686-2502 (G.S.)
Abstract: Pressure is one of the most important parameters controlling the kinetics of chemical reactions. The ability to combine high-pressure techniques with time-resolved spectroscopy has provided a powerful tool in the study of reaction mechanisms. This review is focused on the supporting role of high-pressure kinetic and spectroscopic methods in the exploration of nitric oxide bioinorganic chemistry. Nitric oxide and other reactive nitrogen species (RNS) are important biological mediators involved in both physiological and pathological processes. Understanding molecular mechanisms of their interactions with redox-active metal/non-metal centers in biological targets, such as cofactors, prosthetic groups, and proteins, is crucial for the improved therapy of Citation: Orzeł, Ł.; Oszajca, M.; various diseases. The present review is an attempt to demonstrate how the application of high- Polaczek, J.; Por˛ebska,D.; van Eldik, pressure kinetic and spectroscopic methods can add additional information, thus enabling the R.; Stochel, G. High-Pressure Mechanistic Insight into Bioinorganic mechanistic interpretation of various NO bioinorganic reactions. NO Chemistry. Molecules 2021, 26, 4947. https://doi.org/10.3390/ Keywords: kinetics; high-pressure techniques; nitric oxide; iron complexes; porphyrins; heme molecules26164947 proteins; cobalamins
Academic Editors: Marek Chmielewski, Patryk Niedbala and Maciej Majdecki 1. Introduction With this review, we would like to bring the reader’s attention to high-pressure Received: 30 June 2021 molecular sciences and technology in the advancement of which Professor Janusz Jurczak Accepted: 12 August 2021 made a significant impact, both within synthetic organic chemistry and the development Published: 16 August 2021 of instrumentation [1–3]. Professor Jurczak has been a real leader in this field, and for that reason, the authors of this review dedicate it to his honor. In this review, we focus on Publisher’s Note: MDPI stays neutral the mechanistic studies concerning the interaction of NO with complexes of FeII/III and with regard to jurisdictional claims in CoII/III (including metalloproteins and vitamin B12) performed with the application of published maps and institutional affil- high-pressure kinetic techniques. Since this type of study requires specialized equipment, iations. the number of groups dealing with these studies is limited; therefore, herein, we mainly present the studies performed in our group, as well as those that have resulted from our collaboration with other research groups. Pressure as an experimental variable can provide unique information about the mi- Copyright: © 2021 by the authors. croscopic properties of the studied materials and processes. It can be used as a research Licensee MDPI, Basel, Switzerland. tool for investigating the structure, energetics, dynamics, and kinetics of various processes This article is an open access article and reactions at the molecular level, as well as to chemical synthesis and modifications of distributed under the terms and materials to preserve or improve their quality. The pressure range used for such different conditions of the Creative Commons purposes can extend from a few hundred MPa (reaction kinetics) up to GPa (chemical Attribution (CC BY) license (https:// creativecommons.org/licenses/by/ synthesis or modification of materials). High-pressure kinetic and thermodynamic studies 4.0/). for the elucidation of reaction mechanisms are usually limited to 200 MPa [4–6].
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In order to come as close as possible to the “real” mechanism, it is essential to gain as much information as possible about the chemical understanding of the studied system, empirical rate law, activation and reaction parameters, evidence for possible intermediates, and theoretical analysis of the suggested mechanism. Among the usual variables used in experimental kinetic studies (solvent, ionic strength, pH, etc.), the temperature is a very useful parameter. From the temperature dependence of rate constants and application of the transition state theory, the determination of the enthalpy of activation (∆H‡) and the entropy of activation (∆S‡)—parameters required for the reaction free energy profile— is possible. The additional application of high-pressure kinetic techniques can reveal crucial mechanistic information for chemical processes through the construction of volume profiles with experimentally determined volumes of activation (∆V‡). Such profiles not only complement free energy profiles for the studied reactions but enable a chemical picture to be visualized on the basis of partial molar volume changes that occur along with the reaction coordinate with the estimation of the reaction volume (∆V◦) and the difference in partial molar volumes of product and reactant species [7–9]. From a historical point of view, volumes of activation were obtained for organic reactions long before high-pressure methods were applied to inorganic reactions, for which impressive progress in high-pressure inorganic solution chemistry has been made during the past forty years [10,11]. Furthermore, it was especially the inorganic chemistry community that required experimental techniques to study fast reactions on the second, millisecond, microsecond, and nanosecond timescale. These techniques included stopped- flow, flash-photolysis, pulse-radiolysis, T-jump, and NMR high-pressure developments in the pressure range up to 200 MPa. In this review, we have selected the bioinorganic chemistry of nitric oxide as an example to show how high-pressure kinetic and thermodynamic studies can assist the elucidation of inorganic reaction mechanisms on the molecular level and to improve our understanding of the processes significant for catalysis, health, and the environment. Small inorganic redox molecules, such as nitric oxide (NO), dioxygen (O2), or hydro- gen sulfide (H2S), due to their involvement in numerous catalytic, environmental, and biological processes, have been of interest to scientists from various fields of molecular sciences. Among others, all three molecules and their reactive derivatives play diverse roles in various aspects of cell biology and physiology, including metabolism, cellular signaling, and host defense. The bioinorganic chemistry of these redox molecules plays a central role in their biological activity [12–14]. Nitric oxide (NO) is a short-living free radical, and, in contrast to many signaling agents (e.g., various peptides), which rely on receptors where structural relationships determine their function, the chemistry of NO determines its biological roles. There are two distinct reaction types—direct and indirect—which depend on the NO concentration, reactive species formed and reaction kinetics. The direct effects involve interactions of NO itself with biological targets such as redox metal centers, redox-active amino acids, or other radical species. The indirect activity of nitric oxide is mediated by various reactive nitrogen species (RNS). Recognition of the molecular mechanisms for various reaction types by which NO and other RNS can fulfill their biological function is crucial not only for a better understanding of many natural processes but also for planning innovative strategies in health and environmental protection [15–17].
2. High-Pressure Kinetic Techniques Applied to Mechanistic Studies in Coordination Chemistry The fundamental principle behind the concept of performing high-pressure mecha- nistic studies in coordination chemistry in solution is to gain further mechanistic insight on bond formation and bond cleavage reactions, as well as electron transfer reactions, on the basis of partial molar volume changes. Pressure acceleration is coupled to a negative volume of activation, whereas pressure deceleration is coupled to a positive volume of activation, as illustrated in the following two slides (see Scheme1). Molecules 2021, 26, x FOR PEER REVIEW 3 of 24
Molecules 2021, 26, 4947 3 of 24 volume of activation, whereas pressure deceleration is coupled to a positive volume of activation, as illustrated in the following two slides (see Scheme 1).
A Pressure dependence of reactions in solution B Volume Profile
A -1 A + B Δ Δ ‡ Δ ‡ ln(kp/k0) V = Vf - Vr Δ ‡ mol B Pressure acceleration: - V 3 Δ ‡ Vf ‡ A ----- B Δ ‡ [d(lnk)/dP]T = - V /RT ΔV 0 ‡ Δ ‡ Pressure, MPa ΔV = Activation volume Vr A - B
Δ ‡ Reactants Transition State Products
Pressure deceleration: + V Partial molar volume, cm C Reaction coordinate
A – Cycloaddition; B – Ligand Substitution; C – Homolytic Scission [d(lnk)/dP] = -ΔV ‡/RT T
Scheme 1. (A(A) )Schematic Schematic presentation presentation of ofthe the dependence dependence of ln(k of ln(kp/k0p) /kvs.0 )pressure. vs. pressure. (B) Schematic (B) Schematic presentation presentation of a volume of a volumeprofile. profile.
In the the case case of of reversible reversible reactions, reactions, volume volume profiles profiles can can be be constructed constructed on on the the basis basis of theof the measured measured activation activation volumes volumes for forthe theforwar forwardd and andback back reactions, reactions, or the or reaction the reaction vol- volumeume obtainable obtainable from from the the pressure pressure dependence dependence of of the the overall overall equilibrium equilibrium constant constant K. A few examples of volume profilesprofiles are presented inin thethe subsequentsubsequent sections.sections. During the the 1960s 1960s and and 1970s, 1970s, coordination coordination ch chemistsemists took took the the challenge challenge to develop to develop es- peciallyespecially high-pressure high-pressure instrumentation instrumentation to tost studyudy fast fast reactions reactions on on the the stopped-flow, stopped-flow, T- T- jump, flash-photolysis, flash-photolysis, and NMR timescale. Up until until then, then, high-pressure high-pressure instrumentation was available to study slow reactions as a function of hydrostatic pressure up to 2–3 kbar (200–300 MPa) with a half-life longer than 15 min to pressurize the system and allow for temperature andand pressurepressure equilibration. equilibration. In In principle, principle, one one could could use use a commercial a commercial autoclave auto- withclave awith large a Teflonlarge Teflon bulge filledbulge with filled a with solution, a solution, and withdraw and withdraw samples samples from time from to time to timefollow to thefollow progress the progress of the reaction of the reaction as a function as a function of pressure. of pressure. Different types types of of pressurizing pressurizing systems systems exis exist,t, consisting consisting of a of high-pressure a high-pressure pump, pump, the possibilitythe possibility to change to change from from a hydraulic a hydraulic fluid fluidto another to another pressu pressurizingrizing liquid liquid(such (suchas water as waterfor optical foroptical measurements) measurements) with the with help the of helpa Teflon of a bulge, Teflon pressure bulge, pressure gauges, and gauges, a series and of a pressureseries of pressurevalves, all valves, built into all builta compact into a unit compact for easy unit transportation, for easy transportation, as shown in as Figure shown 1 in Figure1[ 18]. Such transportable units were constructed for use at the Brookhaven [18]. Such transportable units were constructed for use at the Brookhaven National Labor- National Laboratory, New York, for flash-photolysis and pulse-radiolysis experiments, for atory, New York, for flash-photolysis and pulse-radiolysis experiments, for pulse-radiol- pulse-radiolysis experiments at the Hebrew University in Jerusalem, and flash-photolysis ysis experiments at the Hebrew University in Jerusalem, and flash-photolysis experiments experiments at the Jagiellonian University in Krakow, Poland. It enabled the performance at the Jagiellonian University in Krakow, Poland. It enabled the performance of high-pres- of high-pressure kinetic experiments practically all around the world. sure kinetic experiments practically all around the world. An optically see-through two-to-four-window high-pressure cell, as shown in Figure2 , can be used to monitor reaction progress as a function of time, temperature, and pressure for slow (dead time ca. 15 min) and fast (flash-photolysis and pulse-radiolysis) reactions in coordination chemistry [18]. Subsequently, a special technique was developed to fill the pill-box optical cell under un-aerobic conditions [19]. In later developments, the same high-pressure cell, but in a four- window version, was used to perform flash-photolysis and pulse-radiolysis experiments as a function of pressure (see further details given below). In further developments, a very compact high-pressure cell was constructed that enabled spectroscopic studies in the UV–Vis–NIR range up to 400 MPa [20]. In this case the pill-box cell could not be employed any longer, but instead round glass or quartz tubes were used to separate the sample solution from the secondary high-pressure fluid (Figure2C). Depending on the extinction coefficient of the sample to be studied, two different sample tubes with 7.8 mm outer diameter were( used:A) for samples with a high extinction coefficient,(B) a tube with an inner diameter of 1–2 mm was used; for samples with a low extinction coefficient, a tube with an inner diameter of about 5.5 mm was used. In both cases, the tubes were sealed
Molecules 2021, 26, x FOR PEER REVIEW 3 of 24
volume of activation, whereas pressure deceleration is coupled to a positive volume of activation, as illustrated in the following two slides (see Scheme 1).
A Pressure dependence of reactions in solution B Volume Profile
A -1 A + B Δ Δ ‡ Δ ‡ ln(kp/k0) V = Vf - Vr Δ ‡ mol B Pressure acceleration: - V 3 Δ ‡ Vf ‡ A ----- B Δ ‡ [d(lnk)/dP]T = - V /RT ΔV 0 ‡ Δ ‡ Pressure, MPa ΔV = Activation volume Vr A - B
Δ ‡ Reactants Transition State Products
Pressure deceleration: + V Partial molar volume, cm C Reaction coordinate
A – Cycloaddition; B – Ligand Substitution; C – Homolytic Scission [d(lnk)/dP] = -ΔV ‡/RT T
Scheme 1. (A) Schematic presentation of the dependence of ln(kp/k0) vs. pressure. (B) Schematic presentation of a volume profile.
In the case of reversible reactions, volume profiles can be constructed on the basis of the measured activation volumes for the forward and back reactions, or the reaction vol- ume obtainable from the pressure dependence of the overall equilibrium constant K. A few examples of volume profiles are presented in the subsequent sections. During the 1960s and 1970s, coordination chemists took the challenge to develop es- pecially high-pressure instrumentation to study fast reactions on the stopped-flow, T- jump, flash-photolysis, and NMR timescale. Up until then, high-pressure instrumentation was available to study slow reactions as a function of hydrostatic pressure up to 2–3 kbar (200–300 MPa) with a half-life longer than 15 min to pressurize the system and allow for temperature and pressure equilibration. In principle, one could use a commercial auto- clave with a large Teflon bulge filled with a solution, and withdraw samples from time to time to follow the progress of the reaction as a function of pressure. Different types of pressurizing systems exist, consisting of a high-pressure pump, the possibility to change from a hydraulic fluid to another pressurizing liquid (such as water for optical measurements) with the help of a Teflon bulge, pressure gauges, and a series of pressure valves, all built into a compact unit for easy transportation, as shown in Figure 1 Molecules[18].2021, 26Such, 4947 transportable units were constructed for use at the Brookhaven National Labor-4 of 24 atory, New York, for flash-photolysis and pulse-radiolysis experiments, for pulse-radiol- ysis experiments at the Hebrew University in Jerusalem, and flash-photolysis experiments at the Jagiellonian Universitywith moving in pistons Krakow, to transmit Poland. the It pressure, enabled as the described performance in more detailof high-pres- in the original sure kinetic experimentsmanuscript practically [20]. all around the world.
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Figure 1. (A) Schematic diagram of transportable high-pressure unit complete with high-pressure cell. (a) Pressure medium reservoir, (b) oil reservoir, (c) to vacuum line, (d) one-way valve, (e) holder for pump handles, (f) holder for high-pressure cell, and (g) wheels for easy transportation. Numbers 1–8: (high-pressureA) valves that enable the pressurization of particular(B) sections of the high-pressure unit. (B) Picture of transportable suitcase. Reproduced from Reference [18], with the permission of Figure 1. (A) Schematic diagramAIP Publishing. of transportable high-pressure unit complete with high-pressure cell. (a) Pressure medium reservoir, (b) oil reservoir, (c) to vacuum line, (d) one-way valve, (e) holder for pump handles, (f) holder for high-pressure cell, and (g) wheels for easy transportation.An optically Numbers see-through 1–8: high-pressure two-to-four-window valves that enablehigh-pressure the pressurization cell, as shown of particular in Figure sections of the high-pressure2, unit. can (beB) Pictureused to of monitor transportable reaction suitcase. progress Reproduced as a function from Reference of time, [18 ],temperature, with the permission and pres- of AIP Publishing. sure for slow (dead time ca. 15 min) and fast (flash-photolysis and pulse-radiolysis) reac- tions in coordination chemistry [18].
(A) (B) (C)
FigureFigure 2. 2. ((AA)) Two-window Two-window opticaloptical high-pressurehigh-pressure cell cell consisting consisting of of 1 cm–thick1 cm–thick quartz quartz windows windows and and sealed sealed by O-by and O- and∆-rings ∆- ringsfor pressures for pressures up to up 200 to MPa. 200 MPa. Usually Usually the pressure the pressure medium medium is water is water and is and thermostated is thermostated by an outerby an copperouter copper coil not coil shown not shownin the diagram.in the diagram. The pill-box The pill-box consists consis of twots of closely two closely fitting fitting quartz quartz cylinders cylinders which which allow allow compression compression of the of solution the solution inside inside the cell. There is a special hole drilled through both cylinders by which the pill-box optical cell can be filled and the cell. There is a special hole drilled through both cylinders by which the pill-box optical cell can be filled and sealed by sealed by turning the two cylinders 180° apart. (B) Four-window optical high-pressure cell with a thermostating copper turning the two cylinders 180◦ apart. (B) Four-window optical high-pressure cell with a thermostating copper coil. (C) Two coil. (C) Two separated cylinders of the pill-box optical cell that make a gastight fit. Reproduced from Reference [18], with theseparated permission cylinders of AIP of Publishing. the pill-box optical cell that make a gastight fit. Reproduced from Reference [18], with the permission of AIP Publishing. Subsequently, a special technique was developed to fill the pill-box optical cell under The limitations in terms of a faster timescale could only be overcome by turning to un-aerobic conditions [19]. In later developments, the same high-pressure cell, but in a stopped-flow techniques by which reactants could be mixed rapidly. This required the four-window version, was used to perform flash-photolysis and pulse-radiolysis experi- construction of a complete stopped-flow device within a high-pressure cell. The details ments as a function of pressure (see further details given below). In further developments, of this construction are shown in Figure3[ 21]. This high-pressure stopped-flow unit was a very compact high-pressure cell was constructed that enabled spectroscopic studies in designed in such a way that the sample syringes contained ca. 2 mL of solution but enabled the UV–Vis–NIR range up to 400 MPa [20]. In this case the pill-box cell could not be em- more than 20 kinetic traces to be recorded with a single filling of the sample syringes [21]. ployed any longer, but instead round glass or quartz tubes were used to separate the sam- ple solution from the secondary high-pressure fluid (Figure 2C). Depending on the extinc- tion coefficient of the sample to be studied, two different sample tubes with 7.8 mm outer diameter were used: for samples with a high extinction coefficient, a tube with an inner diameter of 1–2 mm was used; for samples with a low extinction coefficient, a tube with an inner diameter of about 5.5 mm was used. In both cases, the tubes were sealed with moving pistons to transmit the pressure, as described in more detail in the original man- uscript [20]. The limitations in terms of a faster timescale could only be overcome by turning to stopped-flow techniques by which reactants could be mixed rapidly. This required the construction of a complete stopped-flow device within a high-pressure cell. The details of this construction are shown in Figure 3 [21]. This high-pressure stopped-flow unit was designed in such a way that the sample syringes contained ca. 2 mL of solution but ena- bled more than 20 kinetic traces to be recorded with a single filling of the sample syringes [21]. At the start of the measurements, the receiver syringe was filled with solvent and
Molecules 2021, 26, x FOR PEER REVIEW 5 of 24
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fully emptied by flushing the optical path in an upward direction. The filled sample sy- ringes were then mounted;At the start atof the the end measurements, of the experiment, the receiver the syringe sample was syringes filled with were solvent empty, and fully and the receiver syringeemptied was by flushingfilled with the opticalthe product path in mixture. an upward Under direction. favorable The filled conditions, sample syringes it was possible to werecomplete then mounted; a whole at pressure the end of dependence the experiment, consisting the sample of syringes four werepressures, empty, and between 5 and 150 theMPa, receiver and syringefive kinetic was filled expe withriments the product at each mixture. pressure. Under The favorable dead-time conditions, of it was possible to complete a whole pressure dependence consisting of four pressures, the stopped-flow unit was determined to be 100 ms from the time the step-motor was between 5 and 150 MPa, and five kinetic experiments at each pressure. The dead-time triggered to the timeof thecomplete stopped-flow mixing unit of was the determined reactants towas be 100achieved. ms from the time the step-motor was triggered to the time complete mixing of the reactants was achieved.
(A) (B) (C)
FigureFigure 3. ( A3.) Cross-sectional(A) Cross-sectional diagram diagram of the high-pressure of the high-pressu vessel andre stopped-flow vessel and apparatus. stopped-flow (1) Pressure apparatus. vessel lid,(1) (2)Pressure pressure vessel, vessel (3) lid, high-pressure (2) pressure window vessel, seal (3) assembly, high-pressure (4) high-pressure window sapphire seal window,assembly, (5) step(4) motor,high-pressure (6) screw- drivesapphire mechanism, window, (7) drive (5) shaft, step (8)motor, syringe (6) thrust screw-drive plate, (9)reactant mechanism, syringe (7) pistons, drive (10) shaft, reactant (8) syringe syringes, thrust (11) Kel-F plate, cell block,(9) reactant (12) mixing syringe jet, (13) receiverpistons, syringe, (10) re andactant (14) receiver-syringesyringes, (11) piston.Kel-F (cellB) High-pressure block, (12) mixing stopped-flow jet, (13) instrument receiver as constructedsyringe, byand van (14) Eldik receiver-syringe and co-workers [21 piston.]. Essential (B) High-pressure components, such stopped-flow as syringes and instrument mixing chamber. as constructed (C) Complete unitby attached van Eldik to the and lid ofco-workers the pressure [21]. cell. ReproducedEssential components, from Reference such [21], withas syringes the permission and mixing of AIP Publishing. chamber. (C) Complete unit attached toThe the next lid developmentof the pressure was cell. the applicationReproduced of pulsed-laserfrom Reference flash-photolysis. [21], with the In this permission of AIP Publishing.case, a four-window high-pressure cell was used in a perpendicular way to flash and trigger the optical detection system after a short time delay in the nanosecond time range [18]. The next developmentFlash photolysis was isthe a powerful application technique of pulsed-laser to study the reaction flash-photolysis. mechanism of coordinationIn this case, a four-windowand high-pressure organometallic cell compounds was used in solution,in a perpendicular where the pressure way to variable flash and adds trig- a further dimension to the mechanistic analysis in terms of volume changes associated with the ger the optical detectionformation system of the after transition a short state. time A laser-pulse delay in the disturbs nanosecond the existing time equilibrium range [18]. situation, Flash photolysis is ona powerful which the subsequenttechnique recombination to study the reaction reaction allows mechanism to follow the of kinetics coordination of the studied and organometallicreaction compounds on a micro- in tosolution, nanosecond wh timescale.ere the pressure A typical laser-pulsed variable adds flash photolysisa further setup dimension to the mechanisticis shown in Figure analysis4. in terms of volume changes associated with the A further development was the challenge to perform pulse-radiolysis experiments at formation of the transitionelevated pressurestate. A to laser-puls study the formatione disturbs of the radicals existing that can equilibrium undergo ligand situation, substitution on which the subsequentand electron recombination transfer reactions. reaction This wasallows not an to easy follow task, the since kinetics the optical of quartzthe stud- windows ied reaction on a micro-used in to the nanosecond standard high-pressure timescale. cell A did typical not allow laser-pulsed an electron beam flash to photolysis reach the sample setup is shown in Figurewithin the4. pill-box cell. Therefore, we had to construct a special steel window that consisted
MoleculesMolecules 2021, 262021, x FOR, 26, 4947PEER REVIEW 6 of 24 6 of 24
of a single 8 mm hole that was 13.3 mm deep, in combination with seven 2.3 mm holes at Molecules 2021, 26, x FOR PEER REVIEW4.3 mm deep, to form a metal grid of 0.7 mm steel that enables the electron beam to enter 6 of 24 the high-pressure cell [22]. The construction of the steel window was such that it met the pill-box cell on the flat optical window, allowing for very close contact with the pressure medium. The details of this construction are shown in Figure5A,B.
Figure 4. A four-window high-pressure cell built into a pulsed-laser flash photolysis unit with an optical detection system, using the pill-box cell shown in Figure 2, which allows a perpendicular alignment of the laser beam and optical detection system.
A further development was the challenge to perform pulse-radiolysis experiments at elevated pressure to study the formation of radicals that can undergo ligand substitution and electron transfer reactions. This was not an easy task, since the optical quartz win- dows used in the standard high-pressure cell did not allow an electron beam to reach the sample within the pill-box cell. Therefore, we had to construct a special steel window that consisted of a single 8 mm hole that was 13.3 mm deep, in combination with seven 2.3 mm holes at 4.3 mm deep, to form a metal grid of 0.7 mm steel that enables the electron beam to enter the high-pressure cell [22]. The construction of the steel window was such that it metFigure Figurethe pill-box 4. A four-window4. cellA four-windowon the high-pressure flat optical cell builtwindhigh-pressure intoow, a pulsed-laserallowing for flashcell very photolysis built close unitinto contact with a an withpulsed-laser the flash photolysis unit with an pressureoptical medium. detection system, The details using the of pill-boxthis construction cell shown in Figureare shown2, which in allows Figure a perpendicular 5A,B. alignmentoptical of thedetection laser beam and system, optical detection using system. the pill-box cell shown in Figure 2, which allows a perpendicular alignment of the laser beam and optical detection system.
A further development was the challenge to perform pulse-radiolysis experiments at elevated pressure to study the formation of radicals that can undergo ligand substitution and electron transfer reactions. This was not an easy task, since the optical quartz win- dows used in the standard high-pressure cell did not allow an electron beam to reach the
(Asample) within the pill-box cell. Therefore,(B) we had to construct a special steel window that
Figure 5.Figure (A) Schematic 5. (A) Schematic diagram diagram consistedof the of theelectron electron beam of beam awindow window single for high-pressurehi 8gh-pressure mm hole pulse pulse radiolysis. that radiolysis. was The electronThe 13 electron.3 beam mm enters beam deep, enters in combination with seven 2.3 mm from thefrom right the side. right side.(B) Schematic (B) Schematicholes diagram diagram at of of 4.3the the pill-boxpill-box mm sample sampledeep, cell, cell, showing to showing form the electron the a electronmetal beam and beam lightgrid and beam oflight paths 0.7 beam and mm paths steel that enables the electron beam and thethe irradiated irradiated volume. volume. Reproduced from from Reference Reference [22], [22], with with the permission the permission of AIP Publishing.of AIP Publishing. to enter the high-pressure cell [22]. The construction of the steel window was such that it The system described here was used for all pulse radiolysis experiments performed at The system described here was used for all pulse radiolysis experiments performed Brookhavenmet the National pill-box Laboratory, cell New on York, the using flat the optical Laser Electron wind Acceleratorow, Facility allowing for very close contact with the at Brookhaven(LEAF), and National the Hebrew Laboratory, University New in Jerusalem York, using [22]. Typicalthe Laser kinetic Electron traces Accelerator showing Fa- cilitythatpressure (LEAF), the electron and themedium. beam Hebrew indeed University reaches The the details formamidein Jerusalem of sample this [22]. within Typicalconstruction the kinetic pill-box traces cell areare showing shown in Figure 5A,B. thatpresented the electron in Figure beam6 on indeed a nanosecond reaches timescale. the formamide sample within the pill-box cell are presented in Figure 6 on a nanosecond timescale.
(A) (B) Figure 5. (A) Schematic diagram of the electron beam window for high-pressure pulse radiolysis. The electron beam enters from the right side. (B) Schematic diagram of the pill-box sample cell, showing the electron beam and light beam paths and the irradiated volume. Reproduced from Reference [22], with the permission of AIP Publishing.
The system described here was used for all pulse radiolysis experiments performed at Brookhaven National Laboratory, New York, using the Laser Electron Accelerator Fa- cility (LEAF), and the Hebrew University in Jerusalem [22]. Typical kinetic traces showing that the electron beam indeed reaches the formamide sample within the pill-box cell are presented in Figure 6 on a nanosecond timescale.
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((AA)) ((BB)) FigureFigureFigure 6.6. 6. (( AA(A)) ) TypicalTypical Typical kinetickinetic kinetic tracestraces traces toto to showshow show thethe the accelerationacceleration acceleration ofof of theth thee reactionreaction reaction atat at 100100 100 MPaMPa MPa inducedinduced induced byby by thethe the LEAFLEAF LEAF facilityfacility facility atat at BNL,BNL, BNL, ‡ NewNewNew York.York. York. (( BB(B)) )PlotPlot Plot ofof of lnln lnkkk versus versus pressure, pressure, where where Δ∆ ΔVV‡‡was was calculated calculated from from from the the the slope slope slope of of of the the the linear linear linear dependence dependence dependence on on on pressure. pressure. pressure.
OurOurOur next nextnext challenge challengechallenge was waswas to to constructto constructconstruct a high-pressure aa hihigh-pressuregh-pressure probe probeprobe for a for Brukerfor aa BrukerBruker 400 MHz 400400 NMR MHzMHz machineNMRNMR machine machine with a with widewith a a bore wide wide magnet bore bore magnet magnet and a 9and and cm a cylindricala 9 9 cm cm cylindrical cylindrical bore. The bore. bore. wide-bore The The wide-bore wide-bore probe couldprobe probe 1 131 1513 1715 17 31 31 becouldcould tuned be be tuned fortuned various for for various various isotopes, isotopes, isotopes, such as such suchH, as as C, H,1H, 13N,C,C, 15N,O,N, and17O,O, and andP, with31P,P, with with a pressure a a pressure pressure range range range of 200ofof 200 200 MPa. MPa. MPa. The The The construction construction construction of of thisof this this probe probe probe was was was completed completed completed in in in 1994 1994 1994 (see (see (see Figure Figure Figure7 )[7) 7) 23[23]. [23].]. TenTen Ten yearsyearsyears later,later, later, wewe we werewere were successful successful successful to to to build build build a a narrow-borea narrow-bore narrow-bore high-pressure high-pressure high-pressure probe probe probe that that that could could could fit fit afit standardaa standard standard magnet magnet magnet with with with a a 3.5a 3.5 3.5 cm cm cm cylindrical cylindrical cylindrical bore bore bore (see (see (see Figure Figure Figure8)[ 8) 8) 24[24]. [24].]. TheThe The uniqueunique unique possibilitypossibility possibility tototo exchangeexchange exchange normalnormal normal andand and high-pressurehigh-pressure high-pressure probesprobes probes fromfrom from thethe the bottombottom bottom ofof of thethe the NMRNMR NMR magnet,magnet, magnet, mademade made ititit easyeasy easy toto to performperform perform high-pressure high-pressure high-pressure measurements measurements measurements since since since everything everything everything could could could be be tunedbe tuned tuned in termsin in terms terms of temperature,ofof temperature, temperature, frequency frequency frequency and and and pressure pressure pressure from from from the bottomthe the bottom bottom of the of of magnet.the the magnet. magnet. The BrukerThe The Bruker Bruker Company Com- Com- alsopanypany now also also has now now a high-pressurehas has a a high-pressure high-pressure unit available unit unit av availableailable for their for for range their their ofrangerange NMR of of machines.NMR NMR machines. machines.
FigureFigureFigure 7.7. 7. SchematicSchematic Schematic diagramdiagram diagram ofof of thethe the titaniumtitanium titanium high-pressurehigh-pre high-pressuressure NMRNMR NMR probe-headprobe-head probe-head designeddesigned designed for for aa a wide-wide- wide- boreborebore magnet.magnet. magnet. ReproducedReproduced Reproduced fromfrom from ReferenceReference Reference [[23],23 [23],], withwith with thethe the permissionpermission permission ofof of AIPAIP AIP Publishing.Publishing. Publishing.
MoleculesMolecules2021 2021, 26, ,26 4947, x FOR PEER REVIEW 8 of 24 8 of 24
Molecules 2021, 26, x FOR PEER REVIEW 8 of 24
(A) (B) Figure 8. (A) Cross-sectional view of the high-pressure autoclave with top and bottom plug, sample Figure 8. (A) Cross-sectional view of the high-pressure autoclave with top and bottom plug, sample tube, macor plug and sample coil. (B) Photograph of two narrow bore probe heads: (a) aluminum jackettube, sealing macor the plug double and helix sample used coil. for thermostating, (B) Photograph (b) ofhigh-pressure two narrow vessel, bore (c) probe platform heads: carrying (a) aluminum thejacket autoclave, sealing (d) the capacitors, double helix (e) capacitor used for platfo thermostating,rms, (f) tuning (b) high-pressure rods, (g) high-pressure vessel, (c) connector, platform carrying (h)the thermocouple, autoclave, (d) (i) capacitors, BNC connector, (e) capacitor (j) Pt-100 platforms, connector, (f)(k) tuning copper rods,tubing, (g) and high-pressure (l) wide-bore connector,
(h)adapter. thermocouple, Reproduced (i) from BNC Reference connector, [24], (j) with Pt-100 the connector, permission (k) of copperAIP Publishing. tubing, and (l) wide-bore adapter. (A) (B) Reproduced from Reference [24], with the permission of AIP Publishing. Figure 8.Finally, (A) Cross-sectional a PhD view student of the high-pressure at the University autoclave with of top Frankfurt and bottom plug,am sampleMain constructed a joule- tube,heating macor plugtemperature-jump and sample coil. (B) Photograph cell that of enabled two narrow a bore discharge probe heads: of (a) 20 aluminum kV to “jump” the tempera- Finally, a PhD student at the University of Frankfurt am Main constructed a joule- jacketture sealing of the the solutiondouble helix by used 2–3 for thermostating, °C, followed (b) high-pressure by the relaxation vessel, (c) platform of the carrying studied equilibrium to the theheating autoclave, temperature-jump(d) capacitors, (e) capacitor platfo cellrms, that (f) enabledtuning rods, a(g) discharge high-pressure ofconnector, 20 kV to “jump” the temperature (h)new thermocouple, temperature (i) BNC for connector, pressures◦ (j) Pt-100 up connector, to 200 MPa(k) copper [25]. tubing, The and high-pressure (l) wide-bore cell itself is shown adapter.inof Figure the Reproduced solution 9A, whereas from by Reference 2–3 the [24],C, temperature-jump followedwith the permission by the of AIPcell relaxation Publishing. is shown ofin Figure the studied 9B. The equilibrium latter cell was to the new temperature for pressures up to 200 MPa [25]. The high-pressure cell itself is shown in constructedFinally, a PhD from student Kel-F at the and University had two of opticalFrankfurt wi amndows Main constructed for the photometric a joule- detection of the heatingabsorbanceFigure temperature-jump9A, changes whereas cellas the thata function temperature-jumpenabled a of discharge time, and of 20 twokV cell to Teflon “jump” is shown membranesthe tempera- in Figure by9 whichB. The the latter pres- cell was turesureconstructed of thewas solution transmitted by from 2–3 °C, Kel-F to followed the andinside by th had eof relaxation the two Kel-F opticalof the cell. studied Gold windows equilibrium electrodes for to the were the photometric used for the rapid detection of new temperature for pressures up to 200 MPa [25]. The high-pressure cell itself is shown indischargethe Figure absorbance 9A, whereas of 20 thekV. changes temperature-jump The high-pressure as a function cell is shown cell of inwa time,Figures mounted 9B. and The twolatter on cell Teflona standard was membranes base plate by of whicha the constructedpressureMessanlagen from was Kel-F Studiengesellschaft transmitted and had two optical to the wi (Göttingen,ndows inside for ofthe thephotometricGermany) Kel-F detection cell. T-jump Gold of theinstrument. electrodes In were conclu- used for the absorbancesion,rapid it dischargecan changes be said as a of functionthat 20 very kV. of time, Thesimilar and high-pressure twoeffect Teflons are membranes observed cell was by withwhich mounted a the joule-heating pres- on a standard temperature- base plate of a surejump was transmittedsystem than to the with inside aof laser-heatedthe Kel-F cell. Gold analog electrodes when were inorganicused for the rapidcomplex formation pro- dischargeMessanlagen of 20 kV. The Studiengesellschaft high-pressure cell was (Göttingen,mounted on a standard Germany) base plate T-jump of a instrument. In conclusion, Messanlagencessesit can beof theStudiengesellschaft said type that investigated very (Göttingen, similar are effects studied.Germany) are T-jump observed instrument. with In aconclu- joule-heating temperature-jump sion, it can be said that very similar effects are observed with a joule-heating temperature- jumpsystem system than than with with a laser-heated a laser-heated analog when analog inorganic when complex inorganic formation complex pro- formation processes of cessesthe of type the type investigated investigated are are studied. studied.
(A) (B) Figure 9. (A) High-pressure (temperature-jumpA) cell as designed by Doss et al. High-pressure(B) cell: Figure 9. (A) High-pressure temperature-jump cell as designed by Doss et al. High-pressure cell: A—vesselFigure lid,9. (B—vesselA) High-pressure body, C—steel temperature-jump piston, D—window support, cell as E— designed∆- and O-rings, by G—spaceDoss et al. High-pressure cell: A—vessel lid, lid, B—vessel B—vessel body, body, C—steel C—steel piston, piston, D—window D—window support, support, E—∆ E—- and∆ -O-rings, and O-rings, G—space G—space for T-jump cell, H—∆- and O-ring, J—steel high-voltage connector, K—insulation material, L—circulation coil, and M—high-voltage plug. (B) T-jump cell: 1—upper electrode, 2—deaeration hole, 3—electrode thread support, 4—Kel-F cell body, 5—membrane support, 6—Teflon membrane, 7—optical window, 8—lower electrode, 9—threaded bolt, and 10—support ring. Reproduced from Reference [25], with the permission of AIP Publishing. Molecules 2021, 26, 4947 9 of 24
3. NO Binding to Heme Proteins and Model Iron Porphyrin Complexes Mechanistic studies on the NO binding to iron(II) and iron(III) porphyrin model systems, as well as heme proteins, provided answers to numerous questions related to the influence of the radical character of NO on its reaction mechanism with an iron center, the role of the metal–ligand system, the role of the amino acid residues surrounding the active center, and the protein superstructure. The activation volume parameter (∆V‡), determined in high-pressure stopped-flow or laser-flash photolysis studies, provided information that was particularly important in the process of unraveling the reaction mechanisms of forma- tion and decay of nitrosyl hemoproteins. Ford and co-workers [26] performed systematic hydrostatic pressure (0.1–250 MPa) measurements and determined ∆V‡ parameters for the “on” and “off” reactions with ferric, as well as for “on” reactions with ferrous water-soluble porphyrins (Table1), where TPPS represents the tetrakis(4-sulfonatophenyl)porphinato anion, and TMPS represents the tetrakis(sulfonatomesityl)porphinato anion (Table1).
Table 1. Rate constants and activation volumes for the reactions of selected iron porphyrins and heme proteins with NO.
∆V‡ k (M−1 s−1) ∆V‡ (cm3/mol) k (s−1) off Reference on on off (cm3/mol) III 4− 5 (at 25 ◦C) 2 (at 25 ◦C) Fe (TPPS )(H2O)2 4.5 × 10 +9 ± 1 5 × 10 +18 ± 2 [26] III 4− 6 (at 25 ◦C) 2 (at 25 ◦C) Fe (TMPS )(H2O)2 2.8 × 10 +13 ± 1 9 × 10 +17 ± 3 [26] ◦ ◦ FeIII(TMPS4−)(OH) 7.4 × 103 (at 10 C) −16.2 ± 0.4 1.5 (at 10 C) +7.4 ± 1.0 [27] III 8− 5 (at 25 ◦C) 2 (at 25 ◦C) Fe (P )(H2O)2 8.2 × 10 +6.1 ± 0.1 2 × 10 +16.8 ± 0.4 [28] ◦ ◦ FeIII(P8−)(OH) 5.1 × 104 (at 25 C) −6.1 ± 0.2 11 (at 25 C) +17 ± 3 [28] III 8+ 4 (at 25 ◦C) (at 25 ◦C) Fe (P )(H2O)2 1.5 × 10 +1.5 ± 0.3 26 +9.3 ± 0.5 [29] III 8+ 3 (at 25 ◦C) (at 25 ◦C) Fe (P )(H2O)(OH) 1.6 × 10 −13.8 ± 0.4 6.2 +2.6 ± 0.2 [29] II 4− 9 (at 25 ◦C) Fe (TPPS )(H2O)2 1.5 × 10 +5 ± 1 - - [26] II 4− 9 (at 25 ◦C) Fe (TMPS )(H2O)2 1.0 × 10 +2 ± 1 - - [26] ◦ ◦ metMb 4.8 × 104 (at 25 C) +21 ± 1 29 (at 25 C) +16 ± 1 [30] 5 (at 25 ◦C) (at 25 ◦C) P450cam—resting state 3.2 × 10 +28 ± 2 0.35 +31 ± 1 [31] 6 (at 25 ◦C) (at 25 ◦C) P450cam—camphor 3.2 × 10 −7.3 ± 0.2 1.93 +24 ± 1 [31] ◦ ◦ SR complex in methanol 2.7 × 106 (at 25 C) +6 ± 1 1.8 (at 25 C) -[32] − R-SO complex in ◦ ◦ 3 6 × 104 (at 25 C) −21 ± 4 2.2 × 103 (at 25 C) +7 ± 3 [33] methanol − 6 (at 25 ◦C) 4 (at 25 ◦C) R-SO3 complex in toluene 1.8 × 10 −25 ± 4 1.2 × 10 +7 ± 3 [33]
Molecules 2021, 26, x FOR PEER REVIEW Volume profiles that clearly visualize the position of the transition state can be10 con- of 24 structed based on the obtained activation volumes. Examples of volume profiles con- structed for the ferric TMPS porphyrin are presented in Figure 10 as a function of pH.
(A) (B)
III III IIIIII FigureFigure 10. 10.Volume Volume profiles profiles for for reversible reversible NO NO binding binding to to Fe(TMPS) Fe(TMPS) (A ()A (TMPS)Fe) (TMPS)Fe(H(H2O)2O)2 and2 and (B ()B (TMPS)Fe) (TMPS)Fe (OH)(OH) under under acidicacidic and and alkaline alkaline conditions, conditions, respectively. respectively.
For both ferri– and ferro–diaqua–heme models, positive ΔV‡on values were deter- mined (Table 1) [26]. Due to the six-coordinate nature of ferri–heme complexes, the large positive ΔV‡on values provided support for a dissociatively activated mechanism with the limiting step expressed by Equation (1).