Abstract
The putative substrate-binding site in lipoxygenases is long and internal. There is little direct evidence about how the unsaturated fatty acid substrates enter and move within the cavity in order to position correctly for electron transfer reactions with the catalytic non-heme iron. An EPR spectroscopy approach, with spin labeled fatty acids, is taken here to investigate dynamic behavior of fatty acids bound to soybean lipoxygenase-1. The probes are labeled on carbons 5-, 8-, 10-, 12- and 16- of stearic acid. The EPR-determined affinity for the enzyme increases as the length of the alkyl end of the probe increases, with ΔΔG of −190 cal/methylene. The probes in the series exhibit similar enhanced paramagnetic relaxation by the iron center. These results indicate that the members of the series have a common binding site. All of the bound probes undergo considerable local mobility. The stearate spin labeled on carbon 5 has highest affinity for the lipoxygenase and it is a competitive inhibitor, with Ki 9 μM. Surprisingly, this stearate labeled near the carboxyl end undergoes more local motion than those labeled in the middle of the chain, when it is bound. This shows that the carboxyl end of the fatty acid spin label is not rigidly docked on the protein. During catalysis, repositioning of the substrate carboxyl on the protein surface may be coupled to motion of portions of the chain undergoing reaction.
Keywords: Lipoxygenase, spin label, fatty acid, substrate motion, paramagnetic protein
Lipoxygenase (LOX) enzymes catalyze the first step in one of the major pathways to molecules derived from arachidonic acid. A theme emerging from the medical perspective on different human lipoxygenases is one of positive and negative influences on human health from these molecules (1, 2). Thus, there is much interest in being able to pharmaceutically modulate the activity of selected members of the lipoxygenase family while leaving other members functioning normally (3, 4). Indeed, inhibitors selective for 5-, 12- or 15- arachidonic acid lipoxygenases have been developed (5–7). Lipoxygenases from both plant and animal sources have overall structural similarity with a long internal cavity that passes by the catalytic iron ion, based on available X-ray structures (8–14). Some determinants of substrate binding within this cavity have been examined by mutation and modeling (15–20), but there is little direct experimental evidence about how fatty acids enter or interact with the cavity. In this report, we take a spectroscopic approach, with spin labeled fatty acids, and examine the dynamic behavior of fatty acids bound to soybean lipoxygenase-1 (SBL1), the most studied representative of the family of LOX enzymes. SBL1 is a 13-linoleic acid, or 15-arachidonic acid, LOX.
The most detailed information presently available about substrate disposition within LOX cavities is based on enzyme kinetics and product analyses. The LOX mechanism (21) includes the enzyme with iron in two redox states (22). The rate-limiting step in the catalyzed reaction is stereoselective abstraction of a hydrogen atom, a proton coupled electron transfer, from a bisallylic methylene of the substrate. This step is accompanied by reduction and protonation of the ferric-hydroxo-metal center, involves hydrogen tunneling, and exhibits a large kinetic isotope effect (23). Subsequently, oxygen reacts with the delocalized radical intermediate at a position usually two carbons removed from the original site of hydrogen abstraction, giving a fatty acid peroxyl radical. Oxygen addition is usually antara-facial to the hydrogen removed, but there is an exception (24), and in either case, it is highly stereoselective (25, 26). Finally, the peroxyl radical accepts an electron from iron to return the metal center to the ferric-hydroxo form. The substrate cavity is very restricted as it passes iron and a structural basis for the mechanism needs to describe the rearrangements that allow both of the electron transfer steps between fatty acid and metal to occur on effectively opposite sides of the substrate.
Placement of the substrate carboxyl has received much attention in proposals for the molecular basis of catalysis by lipoxygenases. There are two structures of molecular complexes with lipoxygenases that provide input about possible placement of the carboxyl. In the first of these, the carboxylate of an inhibitor (RS75091) is about 3.8 Å from ferrous iron, close enough that it might become a ligand in the ferric enzyme form (10). In the second complex, the carboxylate of the product and activator, 13S-hydroperoxyoctadecadienoic acid (13S-HPODE), lies deeply in the internal cavity of the soybean LOX isoform, SBL3, and there it interacts with Arg726 (equivalent to Arg707 in SBL1) (12). The peroxidate is a ligand to ferric iron in this structure. Models of LOX-bound substrate with similar carboxyl placements have been proposed (12, 19, 27, 28). On the other hand, lipoxygenases are also reactive with esters of fatty acid substrates (15, 29) and these substrates are not expected to coordinate iron or form ionic interaction with a buried arginine. A different category of model places the polar end of substrate near the protein surface, close to one suggested entrance to the cavity in SBL1 between Thr 259 and Leu541 (9). In this arrangement, the hydrophobic end of the substrate lies deeply in the binding pocket (18, 20), as shown in Figure 1, essentially in the reverse orientation from that of product in the purple lipoxygenase structure (12). In fact, the stereochemistry of products from double dioxygenations of arachidonic acid demonstrates that substrates can position correctly for catalysis in two orientations: with the methyl end of the substrate chain entering the cavity most deeply or, alternatively, with the carboxyl end entering deepest (20). The former is preferred for the single dioxygenation reactions. The dual orientation option may help explain mixed modes of enzyme inhibition by substrate analogs (30).
A major hydrophobic contribution to binding is apparent from experiments with LOX substrate analogs. Highly specific inhibitors of rabbit 15-LOX (RS75091, Ki=3 μM, (10)) and leukocyte 12-LOX (varied structures with Ki=0.035 to >2 μM, (5)) are substrate-length molecules with selectively placed aromatic rings and alkynyl groups. In other studies, it is shown that the effectiveness of n-alcohols of two to twelve carbons, or related molecules with alkyl chains of similar length, as weak inhibitors of SBL1, increases as the chain length, to about ten carbons (31–33).
To bridge the gap between X-ray structures and modeling, we take a spectroscopic approach to establish determinants of fatty acid binding to SBL1 with a series of spin labels, doxyl stearic acids, DSAs (34). For comparison, interactions of the DSA probes with a different iron-containing enzyme that converts lipoxygenase products, coral allene oxide synthase (cAOS) (35), was examined also. Spin labels are versatile in the ways they can be applied. Electron paramagnetic resonance (EPR) spectra are examined here to map the affinity of the series of DSA molecules for SBL-1, to detect proximity of DSA spin and iron, and to evaluate motion of the probes within the binding site. We find that a stearate labeled near the carboxyl is more mobile in the binding site than other members of the series labeled nearer the middle of the fatty acid chain, and all probes undergo some motion within the binding site.
MATERIALS AND METHODS
Spin label (doxyl-) stearic acids (DSAs) were obtained from Avanti Polar Lipids (Alabaster, Alabama) or were available locally from synthesis (34). The spin label 1-oxyl-2,2,6,6-tetramethyl-4-piperidinol (TEMPOL, both 14N and 15N derivatives) was prepared locally as described (34). Soybean lipoxygenase-1 was purified as described (36) except the anion exchange medium was DE-53 (Whatman) and a high pressure liquid chromatography step was omitted. Expression and purification of C-terminal His-tagged c-AOS was as described (37). Data fits were performed using fitting options available in KaleidaGraph (Synergy.com) and appropriate equations, or, in the case of kinetics, VisualEnzymics (Softzymics.com).
Solubility of Spin Label Fatty Acids
The solubilities of DSA molecules were determined using serial dilutions of each label in working buffer and the intensity of the sharp three-line EPR spectrum was monitored. All of the DSA spin labels were soluble in 2 mM sodium hydroxide and stock solutions prepared thus were stored in plastic. Concentrations of the stock solutions were determined by comparison of double integrals of EPR spectra of the stock DSA solution and a solution of accurately weighed TEMPOL. Stock DSA solutions were diluted into 0.1 M CHES, pH 10, to the desired concentration. Further 1:1 dilution of DSA solution with 0.2 M TRIS (pH 8.35) gave final solutions for solubility determination by EPR in 0.1 M TRIS, 0.05 M CHES (pH 8.4). The stearate spin labels examined are the 5-, 8-, 10-, 12- and 16-doxyl derivatives. The maximal solubility of each label, the cmc, is taken as the highest concentration at which the EPR signal intensity as a function of label concentration is linear. The estimated values of cmc (mM) at pH 8.4 determined in this manner are 0.03 (5-DSA), 0.09 (8-DSA), 0.2 (10-DSA), 0.4 (12-DSA) and 0.1 (16-DSA). These values are given as estimates because substantial errors were encountered in making accurate dilutions of DSA molecules over a wide concentration range, presumably because fatty acids have some affinity for all surfaces (38).
Determination of Dissociation Constants
The dissociation constant, Kd, for different DSA spin labels from SBL1 was determined using a constant DSA concentration and variable protein concentrations. The relative concentrations of free 14N DSA were determined in each protein-containing sample by comparison with the amplitude of the same 14N DSA in buffer without protein. The real concentration of the solution of each 14N DSA in buffer without protein was determined by comparison of double integrals with double integrals of a solution of accurately weighed 14N TEMPOL. An internal standard of 15N TEMPOL was included in titration samples as a convenience in determining relative concentrations of free 14N DSA with varied amounts of SBL1. Protein, spin label and the standard were mixed immediately before each measurement. EPR signal amplitudes did not decrease within the preparation and recording time (less than 30 min). The concentration of bound DSA was taken as [total DSA-free DSA]. At each protein concentration, three measurements were taken. The data were fit to: (Fraction bound) =[P]/(Kd + [P]), where [P] is the protein concentration at each point.
EPR Spectroscopy
Instrumentation: X-band EPR spectra were obtained with a Varian E109 spectrometer equipped with an Oxford Instruments pumped, liquid helium flow cryostat. All low temperature samples, in sealed 50 μl glass microcapillaries, were held in X-band quartz EPR tubes (4 mm OD) containing 99% glycerol, for temperature stability. At X-band, the microwave frequency when the outer tube contained glycerol was 9.2594 ± 0.0001 GHz. Samples for room temperature (295 K) EPR were in 50 μl capillaries held in an outer, 4 mm quartz EPR tube filled with air. In this case, the frequency was 9.2613 ± 0.0001 GHz. Other parameters of X-band recording are specified in figure legends and table footnotes.
Samples
Samples were prepared either in 0.1 M Tris, 0.05 M CHES (pH 8.4) or in 0.1 M Tris, 0.05 M borate (pH 8.7) (see Figure legends). Glycerol was not added to samples unless specified.
Progressive power saturation
The peak-to-peak amplitude of the center line (corresponding to nitrogen nuclear spin mI=0) in the EPR spectra of DSAs bound to either SBL1 or to cAOS was recorded for varied microwave powers. Separate power saturation experiments were examined with samples at temperatures of 20, 40, 60, 80, 100 and 120 K. The power saturation samples were prepared as above, at pH of 8.4, but glycerol was added to 25 %. The value of P1/2 was determined by fitting data acquired from 0.01 to 100 mW to Equation 1, allowing b to float in determining the best fit (39). In Eq. 1, P is the incident power, P1/2 is the power at which the signal intensity is half the value predicted from linear behavior at low power, and K is a constant.
[1] |
Enzyme Kinetics
Kinetics experiments were performed on a Cary 50 UV-Vis spectrophotometer with RX 2000 stopped-flow mixing accessory (Applied Photophysics). One syringe contained substrate and DSA at varied concentrations in 0.1 M sodium borate, pH 10. The other syringe contained 35 nM SBL1 in the same buffer. Equal volumes were mixed. The SBL1 solutions were made up immediately before each run from a 30 μM stock solution in 10 mM sodium acetate, pH 4.6. Data from the first two shots were discarded, and the results of the next three were averaged. The reaction rates were measured at the maximum of the reaction progress curve. Under these conditions, the maximal rate was obtained in 1.5 to 3 s.
RESULTS
Restricted Motions of Spin LabeledStearates Bound to SBL1
All of the stearate spin labels (DSAs) examined gave EPR signals indicating some degree of immobilization upon incubation with lipoxygenase (Figure 2). The ratio of DSA to protein (0.25) was chosen to minimize interaction with weak binding sites, if any. The degree of immobilization, reflected in the separation of low-field maxima and high-field minima in the spectra (2A||′), varied. The vertical lines drawn in Figure 2 are at the magnetic fields of the low and high field extrema in the EPR spectrum of bound 5-DSA. The separation of these extrema, shown in Figure 2 for the 5-DSA spectrum, is called 2A||′. The value of 2A||′ from the spectra of bound 8-, 10- and 12-DSA labels is larger than that for the 5-DSA spectrum (larger separation of outer extrema). The range of values of 2A||′ for the spectra shown in Figure 2 is from 6.00 to 6.36 mT (Table 1). An entry for the EPR spectrum of 16-DSA is not included in Table 1 because a unique separation, 2A||′, cannot be distinguished. The entries for cAOS are commented later.
TABLE 1.
SBL1 100 K 2Azz (mT) | SBL1 295 K 2A||′ | SBL1 295 K A||′/Azz | cAOS 100 K 2Azz (mT) | cAOS 295 K 2A||′ | cAOS 295 K A||′/Azz | |
---|---|---|---|---|---|---|
5-DSA | 7.09 | 5.99 | 0.84 | 7.01 | 5.39 | 0.77 |
8-DSA | 7.00 | 6.17 | 0.88 | 7.04 | 6.07 | 0.86 |
10-DSA | 7.01 | 6.20 | 0.88 | 6.87 | 6.27 | 0.91 |
12-DSA | 6.86 | 6.18 | 0.90 | 6.96 | 6.18 | 0.89 |
16-DSA | 6.95 | 7.03 |
Proteins (1.1 mM) and spin label (0.25 mM) are in 0.05 M CHES and 0.1 M Tris (pH 8.4). Estimated error in values of 2Azz or 2A||′ is ± 0.02 mT. A value of 2A||′ could not be determined for 16-DSA.
Samples prepared in the same manner as for Figure 2 were also examined in the frozen state to determine the rigid limit values of the outer splittings, 2Azz. There are small differences among the DSA molecules bound to SBL1 in the rigid limit 2Azz value, with 5-DSA having the largest (7.08 mT) and 12-DSA the smallest (6.88 mT) values. These differences suggest that the polarity of the immediate environment of the DSA molecules decreases in the order 5-DSA>8-DSA≈10-DSA>16-DSA>12-DSA. Using the ratio A||′/Azz, also given in Table 1, allows the effects of motional averaging on different room temperature spectra to be compared in a polarity-free manner. In the absence of motion, the ratio is one.
Hydrophobic Interactions of Spin LabeledStearates with SBL1
Inspection of Figure 2 reveals that, in the EPR spectra of DSAs labeled on carbons 5, 8, 10 and 12, the intensity of the sharp signals from unbound DSA increases as the number of methylenes between the carbon bearing the label and the terminal methyl decreases. 16-DSA is an exception to this trend and probably has a mode of binding different from the rest of the series. Dilution of samples giving the spectra in Figure 2 gave new EPR spectra in which the fraction of free signal was increased, indicating that the free and bound spin labels are in reversible equilibrium. A fixed concentration of 5-, 8-, 10- or 12-DSA was titrated with SBL1 to determine the values of the dissociation constants, Kd (Figure 3, Table 2). We found less scatter in the binding data when titrations were performed with constant DSA concentration (variable protein concentration) rather than with constant protein concentration (variable DSA concentration), presumably because fatty acids have some affinity for surfaces used in aliquoting (38). Because different constant total spin label concentrations were used in the various titrations, the combined data in Figure 3 are expressed in terms of percent of total label bound, so that the four curves can be compared readily. The inset in Figure 3 gives log (Kd) vs. the number of -CH2- groups between the carbon bearing the doxyl ring and the methyl end of the molecule for the series 5- to 12-DSA. The best fit to the points is the line shown, with slope log (Kd)/methylene = −0.14, or ΔΔG = −190 cal/methylene beyond the position of the doxyl ring.
TABLE 2.
Kd (μM) | log (Kd) | |
---|---|---|
5-DSA | 10 ± 1 | −5.0 |
8-DSA | 31 ± 2 | −4.5 |
10-DSA | 59 ± 2 | −4.2 |
12-DSA | 88 ± 5 | −4.1 |
The DSA concentration was held constant and the SBL1 concentration was varied. The DSA concentrations were 16 _M (5-DSA), 24 _M (8-DSA), 23 _M (10-DSA) and 22 _M (12-DSA). The Kd and errors were determined by fits to experimental data (Figure 3) as outlined in Materials and Methods.
Relaxation of theDoxyl Spin by Iron
Native lipoxygenase contains high spin ferrous iron. Increased relaxation rates are expected if a spin label bound to a protein is close to a fast relaxer, such as iron. Continuous-wave EPR power saturation curves of 5-DSA bound to SBL1, of a water soluble spin label in the presence of SBL1, and of BSA as a non-paramagnetic control, were determined by EPR over the range 20–120 K and the 60 K data are given in Figure 4. Saturation data for another high-spin ferric enzyme with a fatty acid substrate, cAOS, is also shown. Values of P1/2 were determined by curve fits (Materials and Methods). The value of P1/2 is higher for the iron-containing proteins than for BSA at all temperatures, as expected. At 60 K, the P1/2 value determined for 5-DSA bound to SBL1 is 0.61 mW and that for BSA is 0.10 mW; the P1/2 value for cAOS is 0.57 mW; and for comparison, P1/2 is 0.07 mW for the spin label TEMPOL in a solution of SBL1. At 100 K, the P1/2 values were three times larger for the paramagnetic proteins than for BSA. At 20 K, the difference was about an order of magnitude. The values of the exponent b in the curve fits varied from, 1.0 to 1.2 and the errors in P1/2 value are ~10% (Equation 1). Saturation of other DSA molecules, 8-, 10-and 16-DSA, by SBL1 iron was also examined at 100 K (data not shown). Significant differences between P1/2 values of the DSA molecules were not observed.
Another test of proximity of spin label and iron is to determine if dipolar splitting is observed in very low temperature EPR spectra (40). EPR spectra of 5-, 12- and 16-DSA were examined in the temperature range 5–20 K. Some line broadening was observed at the lowest temperature, but no resolved splitting was seen.
Spin Labeled Stearates as Inhibitors ofLipoxygenase
Inhibition, by 5-DSA, of SBL1 oxidation of linoleic acid was examined at pH 10 (0.1 M sodium borate), using substrate and spin label solutions without detergents. Figure 5 shows representative reaction progress curves, and a computer fit to data, for reactions of SBL1 with linoleic acid in the presence and absence of 5-DSA. The data shown in Figure 5b were obtained from kinetic traces (three each) with 0, 2, 4 and 8 μM 5-DSA and a 16.7-fold concentration (3–50 μM) range of linoleic acid, using 17.5 nM SBL1. The available range of 5-DSA concentrations was limited by the solubilities of the mixed fatty acids and rigorous proof of a mode of inhibition could not be obtained. As an example, the data in Figure 5 are fit to a competitive model which, compared to an uncompetitive model, produces a slightly better fit (χ2 is 0.48 and 1.09 for competitive and uncompetitive models, respectively). The parameters of the best fits to the two models are: competitive model: Vmax, 4.7 ± 0.2 μM/s; Km, 17 ± 2 μM; Ki, 9 ± 1.5 μM, and uncompetitive model: Vmax, 5.4 ± 0.4 μM/s; Km, 26 ± 4 μM; Ki, 18 ± 5 μM. The other DSA molecules were also examined by kinetics, but significant inhibition was not observed.
In control experiments, kinetics curves were obtained with and without 1 mM TEMPOL added to linoleic acid (5–80 _M). The kinetics parameters were the same, so it is unlikely that free radical reactions with a nitroxide are the source of inhibition by the DSA spin label. Although there is some leakage of substrate radicals from reactive intermediates in the lipoxygenase reaction (41), the EPR signal of 5-DSA (20 _M) is not reduced within 5 min when linoleate (40 _M) and SBL1 (17.5 nM) are combined.
Spin LabeledStearates Bound to Coral AOS
Dynamics and affinity of the DSA spin labels with cAOS, were surveyed also (Figure 6), for comparison with the study of the affinity of these spin labels for SBL1. Differential motion of stearate chains labeled at various positions is even more pronounced in the case of cAOS compared to SBL1. The range of 2A||′ (295 K) is 5.40 mT to 6.19 mT for the various labels bound to cAOS. The corresponding values of 2A||′/2Azz for 5- and 10- DSA are 0.77 and 0.91 (Table 1). As with SBL1 binding, the mobility of bound spin label is greatest when the doxyl group is at either end of the chain. However, the affinity pattern through the series was different from the regular changes with alkyl chain length observed in DSA binding to SBL1. Stearates 5- to 10-DSA had uniformly high affinity, and 12- and 16-DSA affinities were reduced.
DISCUSSION
A somewhat counterintuitive picture emerges from this spectroscopic study of fatty acid binding to the 13/15-lipoxygenase, SBL1: a trend toward lower affinity correlates with stronger immobilization of the bound probe in a series of doxyl stearic acids, 5- to 12-DSAs. Stearate chains labeled on carbons 8 to 12 are immobilized to a greater extent than when the doxl group is on C-5, but 5-DSA has the highest affinity (Tables 1 and 2). For this to be remarkable, it must be shown that the binding sites for the probes overlap. After a paragraph evaluating the degree of motion, the ensuing paragraphs discuss the evidence pointing to a common binding site. At the outset, it is also noted that the affinity of 16-DSA is higher than expected by extrapolation from results with other members of the series and the motional freedom of this probe is unusually high. Data for 16-DSA are best interpreted in terms of a different mode of binding from the other DSAs.
The 5- to 16-DSA molecules examined here clearly undergo some local motion in their binding sites on SBL1, in addition to reflecting overall tumbling of the protein. A qualitative measure of motion is obtained by comparing the ratio, 2A||′/2Azz, of separation of the outer extrema in the EPR spectra of bound molecules for samples in solution and in frozen (rigid limit) forms (Table 1). The rotational correlation time for a hydrated spherical protein the molecular mass of SBL1 (94 kDa), in aqueous buffer at 293 K, is approximately ~39 ns ((molecular weight/2.4) ns (42)). The lipoxygenase structure has an axial ratio more like 2:1. The effects of diffusional anisotropy limit quantitative analysis of motion because the relation of the probe molecular principal axes to the diffusion axes is not known. However, a calculation appropriate for isotropic diffusion may be taken as a point of reference. The spin label EPR ratio A||′/Azz and the rotational correlation time τR, taking a commonly used Brownian diffusion model of spherical protein motion, are related by Equation 2(43,44).
[2] |
The ratio, A||′/Azz varies from 0.85 to 0.90 in the 5- to 12-DSA series, corresponding to rotational correlation times, by Equation 2, of 6.9 ns (5-DSA) to 12.1 ns (12-DSA). Clearly, even considering SBL1 molecular anisotropy, each of the DSA molecules bound to SBL1 undergoes some local motion, in addition to reflecting overall protein diffusion, and 5-DSA is most mobile within its site, of the 5- to 12-DSA molecules. For comparison with the SBL1 data, the predicted (as above) and EPR-determined (pH 7.0 (45)) rotational correlation times of 12-DSA bound to BSA are ~28 and 30 ns, respectively. A further comparison can be made with 10-DSA bound to cAOS (43 kDa), for which the A||′/Azz value is 0.91 and the EPR-determined and predicted correlation times are 14 ns and 18 ns, respectively. These comparisons emphasize the evident motion of the DSA probes in the binding site on SBL1.
Although the nitroxide rings sense differences in nearby polarity, two forms of evidence point to a common overall binding site for the 5- to 12-DSA series. First, the EPR-derived Kd values vary in a regular way in this series, with a common free energy per methylene on the methyl side of the spin label ring of ΔΔG= ~ −190 cal/methylene. Second, progressive power saturation, which is related to the distance between the nitroxide and the fast relaxing iron, is essentially the same for all the DSA molecules. A working model consistent with these data is shown in Figure 7. The model gives a representation of a binding site on SBL1, and the region shown would correspond to a small region of the whole protein. In the model, the doxyl rings of 8-, 10- and 12-DSA are lodged at the entrance to a restricted cavity that leads to iron. The enhanced mobility in the binding site for 5- and 16-DSA molecules suggests that the hydrocarbon regions of 5- and 16-DSA are too long to get completely into the binding site and fluctuate around the entry. To explain why 16-DSA does not follow the trend in Kd exhibited by the others and that the spin undergoes considerably more motion, the molecular orientation of 16-DSA in the binding site is proposed to be opposite that of the other DSA molecules. Since 12-DSA does not appear to adopt the same orientation as 16-DSA, it may be that the carboxyl of 16-DSA is deep enough in a cavity to form an ionic interaction that would not be available to the shorter carboxyl end of 12-DSA. These considerations raise the possibility that the 16-DSA carboxyl forms a charge interaction with iron. However, a binding site for 16-DSA that is completely different from that occupied by the other DSAs cannot be ruled out.
No dipolar split features were apparent in EPR spectra of DSA labels bound to SBL1 at very low temperature (5–10 K) (40). The iron in resting SBL1 is high spin ferrous (S=2) and thus expected to have zero field splitting (zfs) large compared to the X-band EPR energy. The expectation is that fast relaxation of the metal spin will be dominated by separation of ground and excited states, or by an Orbach process, in the temperature range ~5 to 100 K, as it is for high spin ferric iron with large zfs (46). In high-spin, spin-labeled porphyrins (S=5/2) that also have large zfs, a distance between nitroxide and iron of 11 to 15 Å resulted in resolved dipolar splitting in cw EPR spectra in the 6–8 K temperature range (40). This would seem to rule out the possibility that 5-DSA is able to bind with the carboxyl deep in the SBL1 cavity because that location would place the nitroxide very close to iron. Progressive saturation at 60 K of 5-DSA gave a ratio of P1/2 values of more than eight for the probe on SBL1 compared to TEMPOL in an SBL1 solution, but not bound. Additionally, the half saturation values measured at 100 K for 5- 8-, 10- and 16-DSA bound to SBL1 are identical, within the limits of this kind of measurement. Relaxation of radicals by ferrous iron in photosystems provides examples that may be used to estimate an upper bound to the distance of the DSA spins from ferrous iron in SBL1 (39). The ratio of P1/2 with and without a relaxation contribution from iron, at 30 K, is about eight for the primary acceptor, pheophytin, in photosystem II (47). This radical is 20 ± 4 Å from iron (47). The relaxation mechanism for the DSA spin labels on SBL1 has not been examined in detail yet, and the radicals in the two systems may have different inherent T1s, but it is reasonable to suggest that the spin of 5-DSA has a distance to SBL1 iron that is similar to the pheophytin-iron distance in PSII. Such a distance is compatible with the spin label ring being positioned near the putative cavity entrance between Thr259 and Leu541; for instance, the distance from iron to Leu541 Cβ is 12.5 Å and to Ser261 Oγ is 18 Å.
The Kd of 5-DSA with ferrous SBL1, determined by EPR, is ~10 _M, while Km for linoleate substrate is ~15 _M, suggesting that 5-DSA might be effective as an inhibitor. Indeed, 5-DSA competitively inhibited SBL1-catalyzed oxidation of linoleic acid with Ki of 9.0 ± 1.5 _M. The values of Kd and Ki need not be the same, and since the primary form of the enzyme under turnover conditions is ferric, this Ki is a measure of affinity of DSA molecules for ferric lipoxygenase, while the EPR-determined binding curve (Figure 2) is for ferrous SBL1. There is precedent for an inhibitor having different affinities for ferrous and ferric 12-lipoxygenase (30). The inhibitor in that case has Ki for ferrous 12-lipoxygenase of 0.07 _M and of 2–4 _M for the ferric enzyme. The other DSA molecules in the series did not significantly inhibit SBL1 turnover. Overall, the inhibition by 5-DSA suggests that some part of the substrate-binding site is the binding site for this spin label.
Interactions of the spin labeled fatty acids with coral allene oxide synthase, cAOS (35), were examined for comparison with data from SBL1. The substrate of cAOS is the hydroperoxide product formed by its partner 8R-LOX. The substrate cavity in cAOS is U-shaped and the distance from the surface to the heme iron, about 13 Å, would place the C-8 -OOH group of the substrate in position to react with the heme (34). The affinity pattern of the DSA series is different for cAOS compared to SBL1 (Figure 6). DSA molecules with alkyl chains of 12 to 8 carbons (5 to 10-DSA) had roughly equivalent affinities for cAOS. However, there are striking differences in motion of the various DSAs when bound. The difference in motion exhibited for 5-DSA compared to 8- and 10-DSA is even larger than it was for this comparison in SBL1 data. With regard to the distance of the DSA spin from iron, the half saturation value of 5-DSA, relaxed by cAOS ferric iron at 60 K, is essentially the same as that value for relaxation of 5-DSA by SBL1 ferrous iron.
There is some information about sites where molecules dock from structures of lipoxygenases. An analogous region is involved in binding the inhibitors RS75091 to reticulocyte lipoxygenase (10) and epigallocatechin to the soybean LOX isoform, SBL3 (48). Referring to the helices of SBL1, this region begins between helices-2 and -11 and extends over the side of metal-binding helix-9 where water is coordinated to iron. Six to eight methylenes can be modeled in a hydrophobic cavity lying between iron and residues on helix-11, Ile538 or Leu541 (18, 20). This hydrophobic region, between the surface and iron, is a likely site for binding an aliphatic chain. In the case of the doxyl stearates, the spin label ring is probably too bulky to pass through a restricted cavity entrance, an example of which might be between Thr259 and Leu541 (9). Thus, for each DSA in the series, increasing numbers of methylenes, those between the carboxyl and the spin label ring, are exposed on the surface as the hydrophobic end of the stearate probe gets shorter. The net free energy per methylene for binding the hydrophobic end of a DSA molecule, ~−190 cal/methylene, is smaller than typical values (~−600–800 cal/methylene) obtained when fatty acids of different total lengths are examined in binding to BSA or other proteins (49). Thus, there must be an unfavorable binding contribution from the portion of the DSA chain that remains on the surface of SBL1. A series of synthetic inhibitors of porcine 12-LOX provides information for comparison (5). These molecules feature a benzene ring para- substituted with a variable length carboxyalkyl on one side and variable length alkyl propargyl ether substituted opposite. With a carboxyalkyl end of fixed length, the contribution to binding from the ether end is about −600 cal/methylene for alkyl chains of 6 to 10 carbons. Longer alkyl chains decreased binding, suggesting a limit to the length of the hydrophobic binding site in this 12-LOX. Adding a methylene on the carboxyalky side also decreased binding substantially.
In both SBL1 and cAOS, 5-DSA has greater amplitude of motion at the label site compared to 8- to 12-DSA. Interaction of a ligand carboxyl with a base is generally featured in discussions of a structure of a ligand-protein complex. Bases available to interact with the carboxyl end of fatty acids have been discussed in reports of X-ray structures of lipoxygenases, and in each case, a lysine or arginine is located near the region that is considered a likely entrance to the internal cavity. Residue Lys260 on helix 2 is near a putative entrance in SBL1, while SBL1 and other lipoxygenases have bases opposite this position in what would correspond to helix 11 in SBL1. The role of Lys260 is uncertain, however, because it has been shown that Lys260Leu has unaltered kinetics (28). Perhaps the bulk of the 5-DSA doxyl ring, separated by only three carbons from the carboxylate, interferes with optimal interaction with a base, compared to the situation for 8-, 10- and 12-DSA. However, given the evident hydrophobic effect in binding thermodynamics of DSA molecules, and the fact that esterified fatty acids are good substrates (15, 20, 29), a specific charge interaction of the polar end of fatty acids with the protein may be relatively unimportant, or dynamic on the EPR time scale (μs to ns), for lipoxygenase substrate/product binding. It is possible that motion of the polar end of a fatty acid between multiple weak binding spots on the surface may assist in driving the hydrocarbon end of the substrate into the non-polar channel and in repositioning the peroxyl radical catalytic intermediate so that it can reoxidize iron.
This study was designed to provide a spectroscopic approach to examining how fatty acids interact with a binding site on lipoxygenases. The data suggest that the spin labeled stearates interact with at least part of the substrate site in SBL1. Studies are in progress, using site directed spin labeling, to determine the location of the DSA spins in relation to defined covalent modification sites by spin-spin interaction and, hence, to determine the entrance to the internal cavity.
Acknowledgments
We thank Gurunathan Laxmikanthan for rendering the images given in Figure 1. This work was supported by NIH Grant GM65268 (B.J.G.).
Footnotes
ABBREVIATIONS: cmc, critical micelle concentration; EPR, electron paramagnetic resonance; LOX, any lipoxygenase; SBL1, soybean lipoxygenase isoform-1; 13S-HPODE, 13S-hydroperoxyoctadecadienoic acid; cAOS, coral allene oxide synthase; doxyl-, 1-oxyl-2,2,5,5-tetramethyloxazolidinyl-; x-DSA, a doxyl stearic acid spin label with doxyl ring on carbon x; TEMPOL, 1-oxyl-2,2,6,6-tetramethyl-4-piperidinol; 2Azz, rigid limit separation of outer extrema in spin label EPR spectra; 2A||′, separation of outer extrema when motion is present; P1/2, the microwave power at which the EPR signal is half the value extrapolated from low power; CHES, 2-(cyclohexylamino)ethanesulfonic acid.
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