Linear dichroism and the orientation of reaction centers of Rhodopseudomonas sphaeroides in dried gelatin films

Aqueous mixtures of reaction centers of Rhodopseudomonas sphaeroides and gelatin were dried to form thin films. Following hydration, these films were stretched as much as two to three times their original length. Polarized absorption spectra showing linear dichroism were obtained for both unstretched and stretched films, with the planes and stretching axes of the films mounted in various geometries relative to the electric vector of the measuring beam. These data were analyzed in terms of the following model: Reaction centers possess an axis of symmetry that is fixed in relation to the reaction center structure. In unstretched films this axis is confined to the film plane and oriented at random within the plane. In stretched films the symmetry axis is aligned with the direction of stretching. In both preparations reaction centers are distributed randomly with respect to rotation about the axis of symmetry. The data are consistent with this model when the analysis acknowledges less than perfect orientation. For perfect orientation in a stretched film the model predicts uniaxial symmetry about the axis of stretching. The approach to this condition was examined with films stretched to different extents. Extrapolation yielded dichroic ratios for the ideal case of perfect orientation, and allowed calculation of the angles between the axis of symmetry and the various optical transition dipoles in the reaction center. This treatment included the two absorption bands of the bacteriochlorophyll ‘special pair’ (photochemical electron donor) in the Q_x region, at 600 and 630 nm, which we were able to resolve in light minus dark difference spectra.     

Skew orientation of biological samples Anacystis nidulans cyanobacteria and their fragments in a polymer matrix.

Anacystis nidulans cyanobacteria and their fragments embedded in unstretched, uniaxial and skew (two axes of stretching forming an angle of 40 degrees) stretched poly(vinyl alcohol) films have been investigated. Polarized absorption spectra for uniaxial and skew stretching samples were measured. Both unoriented and oriented samples were photographed under fluorescence microscope. In skew samples a high degree of cell orientation was reached. Skew deformation of polymer matrix compared to one axis stretching provides better band resolution in polarized absorption spectra of Anacystis nidulans samples. The shapes of absorption components measured in respect to the first and second axis of stretching are different which gives the opportunity to investigate position of various group of chlorophyll molecules in membrane.     

Polarized photoacoustic, absorption and fluorescence spectra of chloroplasts and thylakoids oriented in polyvinyl alcohol films

The polarized photoacoustic, absorption and fluorescence spectra of chloroplasts and thylakoids in unstretched and stretched polyvinyl alcohol films were measured. The intensity ratios of fluorescence bands at 674 nm, 700 nm, 730 nm and 750 nm, and the polarized fluorescence excitation spectra are strongly dependent on light polarization and film stretching. In stretched films, thylakoids exhibit predominantly 674 nm emission. The ratio of photoacoustic signal to absorption is different for light polarized parallel and perpendicular to film stretching. This difference is large in the region of chlorophyll a and carotenoids absorption in which the fluorescence excitation spectra are also strongly dependent on light polarization and film stretching. The observed spectral changes are explained by reorientation of pigment molecules influencing the yield of excitation transfer between different pigments.     

Properties of reaction centers of Rhodopseudomonas sphaeroides in dried gelatin films.: Linear dichroism and low temperature spectra

Methods of preparing dried gelatin films containing purified reaction centers of Rhodopseudomonas sphaeroides are described. The spectral properties of reaction centers in solution are essentially maintained in dried gelatin films. These films are uniform and have excellent optical properties, showing little particulate scattering at temperatures down to about 4K. Film contraction on cooling to 90K is less than 1% in linear dimension. Linear dichroism spectra are reported for films at room and low temperature. Reaction centers show a moderate amount of linear dichroism in unstretched gelatin films; the magnitude of the linear dichroism becomes much greater when the films are stretched. In stretched films, linear dichroic ratios ($\text{A}{}_{\mathrm{\parallel }}\text{A}{}_{\mathrm{\perp }}$; absorbance measured with electric vector parallel and perpendicular to stretching direction) between 1.7 and 2.2 were obtained for the 860 nm absorption band of the bacteriochlorophyll component that undergoes primary photooxidation. The relative polarizations of light-induced absorption changes of reaction centers in stretched films are similar to those reported by Vermeglio and Clayton ((1976) Biochim. Biophys. Acta 449, 500–515) and support their hypothesis that absorbance decreases, maximal near 860 and 810 nm, and an increase near 790 nm are associated with the respective disappearance and appearance of discrete bands characteristic of the reduced and oxidized bacteriochlorophyll dimer. This interpretation is also supported by the polarization of the absolute absorption spectrum near 810 and 860 nm. An absorption band near 540 nm, ascribed to the Q_x transitions of two molecules of bacteriopheophytin in the reaction center, is split at low temperatures into two bands having similar polarizations. This splitting is probably not due to exciton coupling of the two molecules, since excition theory predicts different polarizations.     

The orientations of transition moments in reaction centers of Rhodopseudomonas sphaeroides, computed from data of linear dichroism and photoselection measurements.

Linear dichroism measurements of reaction centers of Rhodopseudomonas sphaeroides in stretched gelatin films have yielded angles that various optical transition moments make with an axis of symmetry in the reaction center. Photoselection experiments have yielded angles that certain transition moments make with each other. We have combined these data so as to compute the orientations of the Qx and Qy transition moments of the two molecules of bacteriopheophytin and of the bacteriochlorophyll special pair (photochemical electron donor) in the reaction center. Orientations are expressed in spherical polar coordinates with the symmetry axis as the pole. We have also computed additional angles between pairs of transition moments. In this treatment we have assumed that the bacteriopheophytins are independent monomers with little or no exciton coupling.     

Arrangement of microfibrils in collagen fibrils of tendons in the rat tail

Summary The microfibrillar arrangement in collagen fibrils of tendons in the tail of the rat was examined by electron microscopy and X-ray diffraction. Fresh and air-dried collagen fibers were examined in unstretched and stretched conditions. The results demonstrate that the microfibrils have a course parallel to the longitudinal axis of the collagen fibrils. The influence of stretching and hydration of the samples on the orientation of fibrils and microfibrils is also assessed.     

The orientations of reaction center transition moments in the chromatophore membrane of Rhodopseudomonas sphareroides, bases on new linear dichroism and photoselection measurements.

Chromatophore membranes from Rhodopseudomonas sphaeroides were oriented by drying suspensions on the surfaces of glass slides, Polarized spectra of light-induced absorption changes were obtained between 500 and 1000 nm. As observed earlier, these spectra showed negative bands, reflecting photooxidation of the bacteriochlorophyll 'special pair' in the reaction centers, centered near 870, 810, 630 and 600 nm. These bands have been designated BY1, BY2, BX1 and BX2, respectively, corresponding to two QY transitions and two QX transitions of the dimeric special pair. We found the BY1 and BX1 transition moments to be parallel (within 20 degrees) to the plane of the membrane, whereas the BX2 moment makes an angle of 55--63 degrees with the plane. Using the photoselection technique we found that the angle between the BY1 and BX1 transition moments is 30 degrees, while that between BY1 and BX2 is 75 degrees. The BX1 and BX2 moments were found to be orthogonal, consistent with the prediction of molecular exciton theory for a dimer. By combining these data, we have calculated the orientations of the transition moments of the bacteriochlorophyll dimer in spherical polar coordinates, with the pole of the coordinate system normal to the plane of the membrane. The orientations of the QY and QX transition moments of the two bacteriopheophytin molecules in the reaction center were also computed in this coordinate system by transforming the data reported by Clayton, C.N., Rafferty, R.K. and Vermeglio, A. ((1979) Biochim. Biophys. Acta 545, 58--68). We have derived the transformation equations for two polar coordinate systems: in one, the pole is an axis of symmetry as defined by the orientations of purified reaction centers in stretched gelatin films (Rafferty, C.N. and Clayton, R.K. (1979) Biochim. Biophys. Acta 545, 106--121). In the other, the pole is normal to the plane of the chromatophore membrane. These two polar axes are approximately orthogonal.     

Conformational analysis of phosphatidylethanol-amine in multilayers by infrared dichroism.

Built-up films of L-alpha-dipalmitoyl phosphatidylethanolamine were prepared. Infrared dichroism was measured for the sample and analysed by a new method. This method has been developed for the determination of the directions of transition moments in a film sample, in which there is an axis of symmetry of perpendicular to the film plane. The directions of transition moments were determined for the six vibrations assigned to the CH2 antisymmetric stretching, CH2 symmetric stretching, CH2 scissoring, C=O stretching, PO2- antisymmetric stretching, and C-C-N+ antisymmetric stretching modes. The results indicate that hydrocarbon chains are inclined at about 75 degrees to the film plane and the polar groups orient parallel to the plane in the builtup film. A structural model of the phosphatidylethanolamine in the built-up film is proposed.     

Orientation of cultured arterial smooth muscle cells growing on cyclically stretched substrates

Arterial smooth muscle cells from rabbit aortic media were grown in first subcultures on hydrophilized and collagen-coated silicone membranes which were then subjected to directional cyclic stretches and relaxations at a frequency of 50 times/min. The membranes were stretched 2, 5 and 10% beyond their resting length. Cells on unstretched and stationary membranes in the same chamber served as controls. The cells which were stretched with an amplitude of 2% remained in random orientation after 14 days of continuously performed cyclic stretching. The cells which were stretched 5% for 12 days orientated at an angle of 61 +/- 9 degrees to the direction of stretching, while the cells which were stretched with an amplitude of 10% for 6 days orientated at an angle of 76 +/- 5 degrees. The cells on the stationary and unstretched membranes remained in random orientation. We were able to confirm that the angle of orientation is reversible, i.e. preorientated cells changed their orientation during application of another stretching amplitude. The results suggest that stretching of the artery wall by blood pulsation may be a factor influencing the orientation of smooth muscle cells within the media of the artery wall and of those smooth muscle cells which proliferate into the subendothelial space after mechanical injury of the endothelium or electrical stimulation of the artery wall. An apparatus is presented which produces cyclic and directional mechanical stimuli similar to those which may occur in the artery wall.     

Orientation of the chromophores in the reaction center of Rhodopseudomonas viridis. Comparison of low-temperature linear dichroism spectra with a model derived from X-ray crystallography

Linear dichroism (LD) and absorption (A) spectra of reaction centers from Rhodopseudomonas viridis included in the native chromatophores or reconstituted in planar aggregates have been recorded at 10 K. The samples were oriented in squeezed polyacrylamide gels and the primary donor P was in the reduced or (chemically) oxidized state. The LD spectra of reaction centers in these two states are in favor of a dimeric model of P in which excitonic coupling between the two non-parallel Q_Y transitions leads to a main transition at 990 nm (parallel to the membrane plane) and another one of smaller oscillator strength at 850 nm (tilted at approx. 60° out of the membrane plane). These assignments are in close agreement with the ones proposed in a previous LD study at room temperature (Paillotin, G., Verméglio, A. and Breton, J. (1979) Biochim. Biophys. Acta 545, 249–264). The main Q_X excitonic component of P has a broad absorption peaking at 620 nm and it corresponds to dipoles exhibiting the same orientation as those responsible for the 850 nm transition. On the basis of the present LD study and of CD data of chemically oxidized-minus-reduced reaction centers, we proposed that the minor Q_X excitonic component of P is oriented close to the membrane plane and absorbs around 660 nm. The two monomeric bacteriochlorophylls exhibit a positive LD for both their Q_Y transitions (unresolved at 834 nm) and their Q_X transitions (resolved at 600 and 607 nm), indicating that the planes of these molecules are only slightly tilted out of the membrane plane. The two bacteriopheophytins exhibit strong negative LD with identical LD/A values for their Q_Y transitions (resolved at 790 and 805 nm) and small positive LD for their Q_X transitions (resolved at 534 and 544 nm), demonstrating that these two molecules are strongly tilted out of the membrane plane with each of the Q_Y transitions tilted at approx. 50° out of that plane. A comparison of these LD data with the structural model derived from X-ray crystallography (Deisenhofer, J., Epp, O., Miki, K., Huber, R. and Michel, H. (1984) J. Mol. Biol. 180, 385–398) clearly suggests that a good agreement exists between the results of the two techniques under the following conditions: (i) the C-2 symmetry axis of the reaction center runs along the membrane normal; (ii) excitonic coupling is present only in the primary donor special pair; and (iii) the direction of the optical transitions of the monomeric bacteriochlorophylls and of the bacteriopheophytins is not significantly perturbed by the interactions among the pigments. In addition, a carotenoid is detected in the isolated reaction center with an orientation rather perpendicular to the C-2 symmetry axis. Finally, a comparison of these data with similar ones obtained on the bacteriochlorophyll a-containing reaction center of Rhodopseudomonas sphaeroides 241 points towards a geometrical arrangement of the chromophores which is indistinguishable from the one observed in the reaction center of Rps. viridis.     

Electron microscopy of fine fibrin clots and fine and coarse fibrin films: Observations of fibers in cross-section and in deformed states

Fine fibrin clots and coarse and fine fibrin films (both ligated and unligated), formed by shrinkage of clots in one dimension, were examined by electron microscopy. Specimens of clots were prepared by critical point drying and by embedding and sectioning; specimens of films were prepared by embedding and sectioning only. In the fine clots, network junctions appeared to be formed by fiber segments in which two or more protofibrils were gently twisted around each other for distances of the order of 200 nm and then diverged to give trifunctional branch points. This topology appeared to be preserved in the fine films. It is proposed that the strength of the junctions is primarily provided by the twisting topology, though reinforced by non-covalent bonding involving the B sites uncovered by thrombin. In coarse films, bundles of protofibrils, lying primarily in the film plane, had diameters of 40 to 200 nm and were gently twisted around each other to form thicker cables. Uniaxial stretching, up to 100%, of either fine or coarse film before fixing caused suprisingly extensive orientation of the protofibrils or bundles. However, random orientation was recovered if a stretched ligated film was allowed to retract to its original dimensions before fixing. In a stretched coarse film sectioned perpendicular to the stretch direction, fiber bundles could be seen in cross-section; these were roughly circular with scalloped edges. The changes with stretching and recovery are discussed in relation to possible mechanisms of deformation and elastic energy storage.     

Orientation response of arterial smooth muscle cells to mechanical stimulation

Arterial smooth muscle cells from rabbit aortic media in primary culture and subculture were grown on hydrophilized and collagen-coated silicone membranes which were then subjected to cyclic and directional stretches and relaxations at a frequency of 60 times/min. The membranes were stretched with various amplitudes ranging from 2% to 20%. Smooth muscle cells on unstretched membranes in the same incubation chamber served as controls. In long-term experiments the stretching and relaxing of the membranes was continued for several days. While the smooth muscle cells grown on unstretched membranes remained in random orientation in all experiments, the cells which underwent mechanical stimulation showed a high degree of orientation. The angle of cell orientation varied in direct relation to the stretching amplitude and became steeper in correlation to the intensity of the mechanical stimulus. The angle of cell orientation was reversible, as preoriented cells changed their orientation when another stretching amplitude was applied. To study the role of cytoskeleton in the process of cell orientation, we examined the behaviour of the intracellular actin filament system. In short-term experiments the smooth muscle cells were exposed for 3 to 12 h to cyclic and directional stretches and relaxations with an amplitude of 10%. We observed a rearrangement of the intracellular actin filament system prior to the orientation of the whole cell bodies. The present study provides evidence that stretching the artery wall by blood pulsation may result in an orientation response of the intracellular actin cytoskeleton and in the orientation of the smooth muscle cells within the media of artery walls.     

Small-angle X-ray scattering studies of fibrin film: comparisons of fine and coarse films prepared with thrombin and ancrod

Measurements of small-angle x-ray scattering have been made on films prepared from fine and coarse (i.e., formed at high and low, respectively, pH and ionic strength) clots of bovine fibrin by osmotic shrinkage or compression in one dimension. Intensity profiles were obtained with pinhole geometry on films stretched up to a stretch ratio of 1.43. In unstretched coarse films, repeat spacings were seen at about 245, 120, and 77-80 A. These peaks can probably be identified with the first, second, and third orders of the well-known fibrin repeat of 225 A. In unstretched fine films, only the 77-80 A spacing was seen. In this case, the first two orders may be weak because the half-staggered arrangement of monomer units giving rise to the 225 A reflection is not reinforced by lateral aggregation of protofibrils; the third order may be strong since the molecular subdomains appear to divide the repeat roughly into thirds. After stretching, the 77-80 A spacing persisted in the meridional direction but almost disappeared in the equatorial. Experiments on unstretched films prepared with ancrod substituted for thrombin gave similar results.     

Orientation of reaction center and antenna chromophores in the photosynthetic membrane of rhodopseudomonas viridis

Whole cells of Rhodopseudomonas viridis were oriented in a magnetic field. The degree of orientation of the cells was determined by using a photoselection technique. In order to deduce the orientation of the antennae and chromophores of the reaction centers with respect to the membrane plane, we performed linear dichroism measurements of absolute spectra and light induced difference spectra linked to states P⁺I and PI^? on oriented cells. These measurements lead to the following conclusions:The antennae bacteriochlorophyll molecular plane is nearly perpendicular to the membrane. The Q_y and Q_x transitions moments of these molecules make respectively angles of 20 and 70°ith the membrane plane. The antenna carotenoid molecules make an angle of 45°ith the membrane.The primary electron donor possesses two transition moments centered respectively at 970 and 850 nm. The 970 nm transition moment is parallel to the membrane plane, the 850 nm transition is tilted out of the plane. Upon photooxidation of this primary electron donor, a monomer-like absorption band appears at 805 nm. Its transition makes an angle smaller than 25° with the membrane. The photooxidation of the dimer also induces an absorption band shift for the two other bacteriochlorophyll molecules of the reaction center. The absorption band shifts of the two bacteriochlorophyll molecules occur in opposite direction.One bacteriopheophytin molecule is photoreduced in state PI^?. This photoreduction induces an absorption band shift for only one bacteriochlorophyll molecule. Finally, the geometry of the dimeric primary donor seems to be affected by the presence of a negative charge in the reaction center.     

The orientations of reaction center transition moments in the chromatophore membrane of Rhodopseudomonas sphaeroides, based on new linear dichroism and photoselection measurements

Chromatophore membranes from Rhodopseudomonas sphaeroides were oriented by drying suspensions on the surfaces of glass slides. Polarized spectra of light-induced absorption changes were obtained between 500 and 1000 nm. As observed earlier, these spectra showed negative bands, reflecting photooxidation of the bacteriochlorophyll ‘special pair’ in the reaction centers, centered near 870, 810, 630 and 600 nm. These bands have been designated BY₁, BY₂, BX₁ and BX₂, respectively, corresponding to two Q_y transitions and two Q_x transitions of the dimeric special pair. We found the BY₁ and BX₁ transition moments to be parallel (within 20°) to the plane of the membrane, whereas the BX₂ moment makes an angle of 55–63° with the plane.Using the photoselection technique we found that the angle between the BY₁ and BX₁ transition moments is 30°, while that between BY₁ and BX₂ is 75°. The BX₁ and BX₂ moments were found to be orthogonal, consistent with the prediction of molecular exciton theory for a dimer.By combining these data, we have calculated the orientations of the transition moments of the bacteriochlorophyll dimer in spherical polar coordinates, with the pole of the coordinate system normal to the plane of the membrane. The orientations of the Q_y and Q_x transition moments of the two bacteriopheophytin molecules in the reaction center were also computed in this coordinate system by transforming the data reported by Clayton, C.N., Rafferty, R.K. and Vermeglio, A. ((1979) Biochim. Biophys. Acta 545, 58–68). We have derived the transformation equations for two polar coordinate systems: in one, the pole is an axis of symmetry as defined by the orientations of purified reaction centers in stretched gelatin films (Rafferty, C.N. and Clayton, R.K. (1979) Biochim. Biophys. Acta 545, 106–121). In the other, the pole is normal to the plane of the chromatophore membrane. These two polar axes are approximately orthogonal.     

Linear dichroism of membrane-bound reaction centers from Rhodobacter sphaeroides: Alterations of the B band induced by site-specific mutations

Low temperature absorption and linear dichroism (LD) measurements were performed on oriented membranes containing wild type Rhodobacter sphaeroides reaction centers, a mutant reaction center with the change Phe M197 to Arg (FM197R), and a double mutant reaction center where, in addition, Gly M203 was replaced by Asp (FM197R/GM203D). The monomeric bacteriochlorophyll band (B), which is highly congested in the wild type reaction center, was separated into two bands in the mutant reaction centers peaking 10 nm (single mutant) or 15 nm (double mutant) apart. This separation arose principally from changes in the interaction of the protein with the L-side monomer bacteriochlorophyll B_L.The ability to separate the B bands is extremely useful in spectroscopic studies. The orientations of the two monomer-type transitions contributing to the B band were similar in all three reaction centres studied, and were asymmetric with respect to the orientation axis, with the transition mostly associated with B_L making a smaller angle with the C₂ axis. Differences in the LD observed in wild type membrane-bound or isolated reaction centers can be ascribed either to differences in shifts of the B transitions or to differences in the orientation axis.     

Orientation of spin-labeled myosin heads in glycerinated muscle fibers.

We have used electron paramagnetic resonance (EPR) spectra to study spin labels selectively and rigidly attached to myosin heads in glycerinated rabbit psoas muscle fibers. Because the angle between the magnetic field and the principal axis of the probe determines the position of the EPR absorption line, spectra from labeled fibers oriented parallel to the magnetic field yielded directly the distribution of spin label orientations relative to the fiber axis. Two spin labels, having reactivities resembling iodoacetamide (IASL) and maleimide (MSL), were used. In rigor fibers with complete filament overlap, both labels displayed a narrow angular distribution, full width at half maximum approximately 15 degrees, centered at angles of 68 degrees (IASL) and 82 degrees (MSL). Myosin subfragments (heavy meromyosin and subfragment-1) were labeled and allowed to diffuse into fibers. The resulting spectra showed the same sharp angular distribution that was found for the labeled fibers. Thus is appears that virtually all myosin heads in a rigor fiber have the same orientation relative to the fiber axis, and this orientation is determined by the actomyosin bond. Experiments with stretched fibers indicated that the spin labels on the fraction of heads not interacting with actin filaments had a broad angular distribution. Addition of ATP to unstretched fibers under relaxing conditions produced orientational disorder, resulting in a spectrum almost indistinguishable from that of an isotropic distribution of probes. Addition of either an ATP analog (AMPPNP) or pyrophosphate produced partial disorder. That is a fraction of the probes remained sharply oriented as in rigor while a second fraction was in a disordered distribution similar to that of relaxed fibers.     

The FMO Protein

In this article I review the history of research on the Fenna-Matthews-Olson (FMO) protein with emphasis on my contributions. The FMO protein, which transfers energy from the chlorosome to the reaction center in green sulfur bacteria, was discovered in 1962 and shown to contain bacteriochlorophyll a. From the absorption and circular dichroism spectra, it was clear that there was an exciton interaction between the bacteriochlorophyll molecules. Low temperature spectra indicated a seven-fold exciton splitting of the Q(y) band. The FMO protein was crystallized in 1964, and the X-ray structure determined in 1979 by B.W. Matthews, R.E. Fenna, M.C. Bolognesi, M.F. Schmidt and J.M. Olson. The structure showed that the protein consisted of three subunits, each containing seven bacteriochlorophyll molecules. The optical spectra were satisfactorily simulated in 1997. In living cells the FMO protein is located between the chlorosome and the reaction centers with the C3 symmetry axis perpendicular to the membrane. The FMO protein may be related to PscA in the reaction center.     

Geometry of DNA–dye intercalation complexes from the study of linear dichroic spectra of stretched films

Films of DNA–dye complexes were combined with films of pure DNA deposited on poly(vinyl alcohol) support and stretched. Reproducible dichroic spectra were obtained after equilibration of the stretched films at 93% relative humidity. Dye diffusion into the supporting poly(vinl alcohol) matrix was eliminated. The long axis of intercalated acriflavine is perpendicular to the DNA helix; proflavine deviates slightly and 9-aminoacridine significantly from such an intercalation geometry. The dichroism of two mutually perpendicularly polarized transitions of 9-aminoacridine enabled us to determine both the angles of tilt and twist of the plane of the dye relative to the DNA helix in the complex.     

Acute effects of static stretching on peak torque in women

The purpose of this study was to examine the effects of static stretching on concentric, isokinetic leg extension peak torque (PT) at 60 and 240 degrees.s(-1) in the stretched and unstretched limbs. The PT of the dominant (stretched) and nondominant (unstretched) leg extensors were measured on a calibrated Cybex 6000 dynamometer. Following the prestretching PT assessments, the dominant leg extensors were stretched using 1 active and 3 passive stretching exercises. After the stretching, PT was reassessed. The results of the statistical analyses indicated that PT decreased following the static stretching in both limbs and at both velocities (60 and 240 degrees.s(-1)). The present findings suggested that the stretching-induced decreases in PT may be related to changes in the mechanical properties of the muscle, such as an altered length-tension relationship, or a central nervous system inhibitory mechanism. Overall, these findings, in conjunction with previous studies, indicated that static stretching impairs maximal force production. Strength and conditioning professionals should consider this before incorporating static stretching in preperformance activities. Future studies are needed to identify the underlying mechanisms that influence the time course of stretching-induced decreases in maximal force production for athletes and nonathletes across the age span.