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Randy W Larsen

Publications and source records attributed to Randy W Larsen.

17 recordsLinked to original sources

Time-resolved thermodynamic profiles for CO photolsysis from the mixed valence form of bovine heart cytochrome c oxidase.

Photoacoustic calorimetry has been utilized to probe the thermodynamics accompanying photodissociation of the CO mixed valence form of bovine heart cytochrome c oxidase (COMV CcO). At pH's below 9 photolysis of the COMV CcO results in three kinetic phases with the first phase occurring faster than the time resolution of the instrument (i.e., < approximately 50 ns), a second phase occurring with a lifetime of approximately 100 ns and a third phase occurring with a lifetime of approximately 2 micros. The corresponding volume and enthalpy changes for these processes are: DeltaH1, DeltaV1 = +79 +/- 10 kcal mol(-1), +9 +/- 1 mL mol(-1); DeltaH2, DeltaV2 = -79 +/- 5 kcal mol(-1), -9 +/- 2 mL mol(-1); DeltaH3, DeltaV3 = +54 +/- 7 kcal mol(-1), +8 +/- 1 mL mol(-1). At pH's above 9 only one phase is observed, a prompt phase occurring in < 50 ns. The overall volume change is negligible above pH 9 and the enthalpy change is +29 +/- 5 kcal mol(-1). The data are consistent with the prompt phase being associated with CO-Fe(a3) bond cleavage, CO-CuB+ bond formation, Fe(a3) low-spin to high-spin transition and fast electron transfer (ET) from heme a3 to heme a followed by proton transfer from Glu242 to Arg38 on an approximately 100 ns timescale. The slow phase is likely a combination of CO thermal dissociation from CuB and additional ET between heme a3 to heme a. Interestingly, this phase is not evident above pH 9 suggesting linkage between CO dissociation/ET and the protonation state of a group or groups near the binuclear center.

Animals↗

Thermodynamics of carbon monoxide photodissociation from the fully reduced cytochrome aa3 oxidase from Rb. sphaeroides.

Photodissociation of the fully reduced carbonmonoxy bound cytochrome aa3 from Rb. sphaeroides results in ultrafast ligand transfer between heme a3 and CuB, which is followed by thermal dissociation from CuB on longer time scales. We have utilized photoacoustic calorimetry to obtain a detailed thermodynamic description of the mechanism of ligand photodissociation and transfer between heme a3 and CuB. Subsequent to ligand photodissociation an additional process, which has not been characterized previously, was observed with the lifetime of 485 ns at 18 degrees C and is coupled to a volume expansion of 3.3 ml mol(-1). From the temperature dependence, an activation barrier of 4 kcal mol(-1) was determined. We attribute the observed 500 ns process to changes in CuB ligation subsequent to ligand translocation. In a photoacoustic study on CO photodissociation from bovine heart aa3 oxidase, no volume changes were observed on the ns timescale, indicating that a different mechanism may control ligand dissociation and binding within the binuclear center of the bacterial and bovine enzymes.

Animals↗

Spectroscopic and photothermal study of myoglobin conformational changes in the presence of sodium dodecyl sulfate.

Interactions between sodium dodecyl sulfate (SDS) and horse heart myoglobin (Mb) at surfactant concentrations below the critical micelle concentration have been studied using steady-state and transient absorption spectroscopies and photoacoustic calorimetry. SDS binding to Mb induces a heme transition from high-spin five-coordinate to low-spin six-coordinate in met- and deoxyMb, with the distal His residue likely to be the sixth ligand. The transition is complete at an SDS concentration of approximately 350 microM and approximately 700 microM for met- and deoxyMb, respectively. DeltaG(H(2)O) and m values determined from equilibrium SDS-induced unfolding curves indicate similar stability of met- and deoxyMb toward unfolding; however, the larger m value for the deoxyMb equilibrium intermediate indicates that its structure differs from that of metMb. Results from transient absorption spectroscopy show that CO rebinding to Fe(2+)-Mb in the presence of SDS is a biphasic process with the rate constant of the first process approximately 5.5 x 10(3) s(-1), whereas the second process displays a rate similar to that for CO rebinding to native Mb (k(obs) = 7.14 x 10(2) s(-1)) at 1 mM CO. Results of photoacoustic calorimetry show that CO dissociation from deoxyMb occurs more than 10 times faster in the presence of SDS than in native Mb. These data suggest that the heme binding pocket is more solvent-exposed in the SDS-induced equilibrium intermediate relative to native Mb, which is likely due to the electrostatic and hydrophobic interactions between surfactant molecules and the protein matrix.

Animals↗

Effects of turn stability on the kinetics of refolding of a hairpin in a beta-sheet.

As part of our continuing study of the effects of the turn sequence on the conformational stability as well as the mechanism of folding of a beta-sheet structure, we have undertaken a parallel investigation of the solution structure, conformational stability, and kinetics of refolding of the beta-sheet VFIVDGOTYTEV(D)PGOKILQ. The latter peptide is an analogue of the original Gellman beta-sheet VFITS(D)PGKTYTEV(D)PGOKILQ, wherein the TS(D)PGK turn sequence in the first hairpin has been replaced by VDGO. Thermodynamics studies revealed comparable conformational stability of the two peptides. However, unlike the Gellman peptide, which showed extremely rapid refolding of the first hairpin, early kinetic events associated with the refolding of the corresponding hairpin in the VDGO mutant were found to be significantly slower. A detailed study of the conformation of the modified peptide suggested that hydrophobic interactions might be contributing to its stability. Accordingly, we surmise that the early kinetic events are sensitive to whether the formation of the hairpin is nucleated at the turn or by sequestering of the hydrophobic residues across the strand, before structural rearrangements to produce the nativelike topology. Nucleation of the hairpin at the turn is expected to be intrinsically rapid for a strong turn. However, if the process must involve collapse of hydrophobic side chains, the nucleation should be slower as solvent molecules must be displaced to sequester the hydrophobic residues. These findings reflect the contribution of different forces toward nucleation of hairpins in the mechanism of folding of beta-sheets.

Amino Acid Sequence↗

Characterization of conformational changes coupled to ligand photodissociation from the heme binding domain of FixL.

Using transient absorption spectroscopy and photoacoustic calorimetry (PAC), we have characterized carbon monoxide photodissociation and rebinding to two forms of the heme domain of Bradyrhizobium japonicum FixL. Transient absorption results for the complete heme domain (FixL residues 140-270) and a truncated heme domain (missing 11 residues on the N-teminal end and 14 amino acid residues on the C-terminal end of the full length heme domain) show similar rates for ligand rebinding to the five-coordinate heme domain and the absence of any transient intermediate on a microsecond time scale. Results from PAC studies show that both the truncated and complete heme domains undergo a contraction upon ligand photolysis. In addition, CO photolysis from the complete heme domain gives rise to an intermediate with a lifetime of approximately 150 ns which is absent in the truncated heme domain. We attribute the 150 ns phase to ligand release to the solvent which may be accelerated in the case of the truncated domain. The initial contraction is attributed to changes in the charge distribution due to reorganization of the surface salt bridge formed between Glu182 and Arg227 or possibly to reorientation of Arg206. Changes in the charge distribution may play an important role in communication between the sensor domain and the regulatory domain and thus may be part of the signal transduction pathway.

Bacterial Proteins↗

Photothermal studies of CO photodissociation from mixed valence Escherichia coli cytochrome bo3.

Here, we report the volume and enthalpy changes accompanying CO photodissociation from the mixed valence form of cytochrome bo3 oxidase from Escherichia coli. The results of photoacoustic calorimetry indicate two kinetic phases with distinct volume and enthalpy changes accompanying CO photodissociation from heme o3 and its transfer to CuB. The first phase occurring on a timescale of <50 ns is characterized by a volume decrease of -1.3+/-0.3 mL mol-1 and enthalpy change of 32+/-1.6 kcal mol-1. Subsequently, a volume increase of 2.9 mL mol-1 with an enthalpy change of -5.3+/-2.5 kcal mol-1 is observed with the lifetime of approximately 250 ns (this phase has not been detected in previous optical studies). These volume and enthalpy changes differ from the volume and enthalpy changes observed for CO dissociation from fully reduced cytochrome bo3 oxidase indicating that the heme o3/CuB active site dynamics are affected by the redox state of heme b.

Carbon Monoxide↗

Thermodynamic profiles for CO photodissociation from heme model compounds: effect of proximal ligands.

Here we present a comprehensive study of the thermodynamic parameters (enthalpy, entropy, and volume changes) associated with carbon monoxide photodissociation and rebinding to Fe(II) microperoxidase-11 (Fe(II)MP11) and Fe(ll) tetrakis(4-sulfonatophenyl)porphine complex (FeII4SP) with water and 2-methylimidazole as proximal ligands. CO photodissociation from FeII4SP complexes is accompanied by a positive volume change of approximately 17 mL mol(-1). A smaller volume change of approximately 12 mL mol(-1) was observed for CO dissociation from Fe(II)MP-11. We attribute the positive volume change to cleavage of the Fe-CO covalent bond and to solvent reorganization due to the low-spin to high-spin transition. CO binding is an exothermic reaction with an enthalpy change of -17 kcal mol(-1) for the CO-FeII4SP complexes and -13 kcal mol(-1) for the CO-Fe(II)MP11 complex. In all cases, the ligand recombination occurs as a single-exponential process indicating that CO dissociation is followed by direct CO rebinding to a high-spin five-coordinate complex without concomitant dissociation of the proximal base. In addition, observed negative activation entropies and volumes for ligand binding to (2-Melm)FeII4SP and MP-11, respectively, suggest that CO rebinding can be described by an associative mechanism with bond formation being the rate-limiting step.

Journal Article↗

Time-resolved photoacoustics study of the ruthenium(II) bis(2,2'-bipyridine)(4,4'-dicarboxy-2,2'-bipyridine) complex.

The formation and the decay of the triplet metal to ligand charge transfer state ((3)MLCT) of ruthenium(II) bis(2,2'-bipyridine)(4,4'-dicarboxy-2,2'-bipyridine) (Ru(bpy)(2)(dcbpy)) were characterized using photoacoustic calorimetry. At pH 6 and 2, the (3)MLCT state formation leads to a volume change of -8 mL mol(-1) and enthalpy changes of 17 kcal mol(-1) and 13 kcal mol(-1), respectively. We attribute the volume contraction to structural changes and to solvent electrostriction. At pH 4, the photoexcitation of the complex leads to an expansion of 14 mL mol(-1) and an enthalpy change of approximately 119 kcal mol(-1) due to protonation of the carboxyl group in the excited state.

Journal Article↗

Measuring the refolding of beta-sheets with different turn sequences on a nanosecond time scale.

Whether turns play an active or passive role in protein folding remains a controversial issue at this juncture. Here we use a photolabile cage strategy in combination with laser-flash photolysis and photoacoustic calorimetry to study the effects of different turns on the kinetics of beta-hairpin refolding on a nanosecond time scale. This strategy opens up a temporal window to allow the observation of early kinetic events in the protein refolding process at ambient temperature and pH without interference from any denaturants. Our results provide direct evidence demonstrating that even a one-residue difference in the turn region can change the refolding kinetics of a peptide. This observation suggests an active role for turn formation in directing protein folding.

Amino Acid Sequence↗

Volume and enthalpy profiles of CO rebinding to horse heart myoglobin.

Carbon monoxide binding to myoglobin was characterized using the photothermal beam deflection method. The volume and enthalpy changes coupled to CO dissociation were found to be 9.3+/-0.8 mL x mol(-1) and 7.4+/-2.8 kcal x mol(-1), respectively. The corresponding values observed for CO rebinding have the same magnitude but opposite sign: Delta V=-8.6+/-0.9 mL x mol(-1) and Delta H=-5.8+/-2.9 kcal x mol(-1). Ligand rebinding occurs as a single conformational step with a rate constant of 5 x 10(5) M(-1) s(-1) and with activation enthalpy of 7.1+/-0.8 kcal x mol(-1) and activation entropy of -22.4+/-2.8 cal x mol(-1) K(-1). Activation parameters for the ligand binding correspond to the activation parameters previously obtained using the transient absorption methods. Hence, at room temperature the CO binding to Mb can be described as a two-state model and the observed volume contraction occurs during CO-Fe bond formation. Comparing these results with CO dissociation reactions, for which two discrete intermediates were characterized, indicates differences in mechanism by which the protein modulates ligand association and dissociation.

Animals↗

Ligand binding subsequent to CO photolysis of methionine-modified cytochrome c.

In this report the kinetics of CO recombination to ferrocytochrome c in which Met80 has been oxidized to a sulfoxide are examined. Transient optical difference spectra suggest that the species formed immediately after photolysis contains a five-coordinate high spin heme. Single wavelength transient absorption data show triphasic kinetics with rate constants of (2.1+/-0.08)x10(4), (2.0+/-0.01)x10(3), and 57+/-0.01 s(-1). The data suggest a model for ligand recombination in which the methionine sulfoxide and CO compete for binding to the five-coordinate heme with rate constants of (2.1+/-0.08)x10(4) and (2.0+/-0.01)x10(3) s(-1), respectively. Carbon monoxide then binds to the population of cytochrome c containing the methionine sulfoxide with a rate constant of 57 s(-1). In addition, the slower than expected rate of methionine sulfoxide recombination (much smaller rate constant than expected for a ligand restricted to the distal heme pocket) is attributed to hydrogen bonding between the unbound methionine sulfoxide and Tyr(68).

Animals↗

A molecular dynamics method for calculating molecular volume changes appropriate for biomolecular simulation.

Photothermal methods permit measurement of molecular volume changes of solvated molecules over nanosecond timescales. Such experiments are an important tool in investigating complex biophysical phenomena including identifying transient species in solution. Developing a microscopic understanding of the origin of volume changes in the condensed phase is needed to complement the experimental measurements. A molecular dynamics (MD) method exploiting available simulation methodology is demonstrated here that both mimics experimental measurements and provides microscopic resolution to the thermodynamic measurements. To calculate thermodynamic volume changes over time, isothermal-isobaric (NPT) MD is performed on a solution for a chosen length of time and the volume of the system is thus established. A further simulation is then performed by "plucking" out a solute molecule of interest to determine the volume of the system in its absence. The difference between these volumes is the thermodynamic volume of the solute molecule. NPT MD allows the volume of the system to fluctuate over time and this results in a statistical uncertainty in volumes that are calculated. It is found in the systems investigated here that simulations lasting a few nanoseconds can discern volume changes of approximately 1.0 ml/mole. This precision is comparable to that achieved empirically, making the experimental and theoretical techniques synergistic. The technique is demonstrated here on model systems including neat water, both charged and neutral aqueous methane, and an aqueous beta-sheet peptide.

Algorithms↗

Kinetics of intramolecular electron transfer in cytochrome bo3 from Escherichia coli.

We have examined the temperature dependence of the intramolecular electron transfer (ET) between heme b and heme o(3) in CO-mixed valence cytochrome bo(3) (Cbo) from Escherichia coli. Upon photolysis of CO-mixed valence Cbo rapid ET occurs between heme o(3) and heme b with a rate constant of 2.2 x 10(5) s(-1) at room temperature. The corresponding rate of CO recombination is found to be 86 s(-1). From Eyring plots the activation energies for these two processes are found to be 3.4 kcal/mol and 6.7 kcal/mol for the ligand binding and ET reactions, respectively. Using variants of the Marcus equation the reorganization energy (lambda), electronic coupling factor (H(AB)), and the ET distance were found to be 1.4 +/- 0.2 eV, (2 +/- 1) x 10(-3) eV, and 9 +/- 1 A, respectively. These values are quite distinct from the analogous values previously obtained for bovine heart cytochrome c oxidase (CcO) (0.76 eV, 9.9 x 10(-5) eV, 13.2 A). The differences in mechanisms/pathways for heme b/heme o(3) and heme a/heme a(3) ET suggested by the Marcus parameters can be attributed to structural changes at the Cu(B) site upon change in oxidation state as well as differences in electronic coupling pathways between Heme b and heme o(3).

Copper↗

Conformational dynamics and temperature dependence of photoinduced electron transfer within self-assembled coproporphyrin:cytochrome c complexes.

The focus of the present study is to better understand the complex factors influencing intermolecular electron transfer (ET) in biological molecules using a model system involving free-base coproporphyrin (COP) complexed with horse heart cytochrome c (Cc). Coproporphyrin exhibits bathochromic shifts in both the Soret and visible absorption bands in the presence of Cc and an absorption difference titration reveals a 1:1 complex with an association constant of 2.63 +/- 0.05 x 10(5) M(-1). At 20 degrees C, analysis of time-resolved fluorescence data reveals two lifetime components consisting of a discrete lifetime at 15.0 ns (free COP) and a Gaussian distribution of lifetimes centered at 2.8 ns (representing (1)COP --> Cc ET). Temperature-dependent, time-resolved fluorescence data demonstrate a shift in singlet lifetime as well as changes in the distribution width (associated with the complex). By fitting these data to semiclassical Marcus theory, the reorganizational energy (lambda) of the singlet state electron transfer was calculated to be 0.89 eV, consistent with values for other porphyrin/Cc intermolecular ET reactions. Using nanosecond transient absorption spectroscopy the temperature dependences of the forward and thermal back ET originating from triplet state were examined ((3)COP --> Cc ET). Fits of the temperature dependence of the rate constants to semiclassical Marcus theory gave lambda of 0.39 eV and 0.11 eV for the forward and back triplet ET, respectively (k(f) = (7.6 +/- 0.3) x 10(6) s(-1), k(b) = (2.4 +/- 0.3) x 10(5) s(-1)). The differing values of lambda for the forward and back triplet ET demonstrate that these ET reactions do not occur within a static complex. Comparing these results with previous studies of the uroporphyrin:Cc and tetrakis (4-carboxyphenyl)porphyrin:Cc complexes suggests that side-chain flexibility gives rise to the conformational distributions in the (1)COP --> Cc ET whereas differences in overall porphyrin charge regulates gating of the back ET reaction (reduced Cc --> COP(+)).

Animals↗

Photothermal studies of pH induced unfolding of apomyoglobin.

Conformational dynamic and enthalpy changes associated with pH induced unfolding of apomyoglobin were studied using photoacoustic calorimetry and photothermal beam deflection methods. The transition between the native state and the I intermediate was induced by a nanosecond pH jump from o-nitrobenzaldehyde photolysis. Deconvolution of photoacoustic waves indicates two kinetic processes. The fast phase (T < 50 ns) is characterized by a volume expansion of 8.8 ml mol(-1). This process is followed by a volume contraction of about -22 ml mol(-1) (tau approximately 500 ns). Photothermal beam deflection measurements do not reveal any volume changes on the time scale between approximately 100 micros and 5 ms. We associate the volume contraction with structural changes occurring during the transition between the native state and the I intermediate. The lack of any processes on the ms time scale may indicate the absence of structural events involving larger conformational changes of apomyoglobin after the pH jump.

Acoustics↗

Aerotactic responses in bacteria to photoreleased oxygen.

Bacterial aerotaxis is a rapid response towards or away from oxygen. Here we report on the use of computer-assisted motion analysis coupled to flash photolysis of caged oxygen to quantify aerotactic responses in bacteria. The caged compound (mu-peroxo)(mu-hydroxo)bis[bis(bipyridyl) cobalt(III)] perchlorate liberates molecular oxygen upon irradiation with near-UV light. A mixture of cells and the caged oxygen compound was placed in a capillary tube and challenged by discrete stimuli of molecular oxygen produced by photolysis. We then recorded the rate of change of direction (rcd) as an estimate of tumble frequency in response to liberated oxygen and measured the signal processing (excitation) times in Bacillus subtilis, Bacillus halodurans and Escherichia coli. This computer-assisted caged oxygen assay gives a unique physiological profile of different aerotaxis transducers in bacteria.

Bacillus subtilis↗