Study design and ethical statement
The present study uses a cross-sectional study design. Ethical clearance was obtained from the Health Research Ethics Committee (HREC) of Stellenbosch University, South Africa (N19/03/043) and from the Ethics Committee of the Medical University Vienna, Austria (EK1371/2015). Written informed consent was obtained from all participants followed by whole blood sampling. Study participants received a unique number that was used to guarantee anonymity throughout this study, and researchers followed Good Clinical Practice and guidelines from the ethics committee.
Participants and blood collection
Healthy volunteers (N=39; 23 females, 16 males; median age [interquartile range]: 42 [21 – 58]) were recruited for this study. The inclusion criteria for healthy volunteers were: non-smokers, absence of infection, no use of anti-inflammatory or chronic medication, and no previous history of thrombotic disease. Blood was drawn in serum‑separating, EDTA and sodium citrate tubes by a phlebotomist. After the blood was drawn, whole blood samples were allowed to rest for 30 minutes at room temperature before further processing for experimentation. Two plasma derivatives were created. Platelet poor plasma (PPP) was created by centrifuging whole blood at 3000g for 15 minutes. The plasma fraction was collected and stored at -80°C until experimentation. For rheometry analysis, platelet-depleted plasma (PDP) was created by centrifuging whole blood at 325g for 8 minutes. After removal of the surface layer, the top two-thirds of this plasma were collected and centrifuged a second time at 2310g for 30 minutes, and the top two-thirds ultimately used for experimentation.
Purified fibrin(ogen) clot model
We used three purified fibrin(ogen) clot models: (1) fluorescent fibrinogen conjugated to Alexa Fluor™488 (ThermoFisher, F13191), (2) non-conjugated purified fibrinogen (Sigma, F3879) and (3) non-conjugated purified fibrinogen depleted of von Willebrand factor, plasminogen and fibronectin (CoaChrom, HFG3).
Scanning Electron Microscopy
Platelet poor plasma with LPS
A scanning electron microscope was used to view the ultrastructural changes of clots. PPP was exposed to LPS from P. gingivalis (n=10; 10 ng.L-1; 30 min) before creating a plasma clot on a 10 mm glass cover slip with the addition of thrombin (7 U·mL-1). Matching naïve clots were prepared with addition of thrombin. The samples were then washed in PBS followed by a fixation step of 4% formaldehyde and secondary fixation in 1% osmium tetroxide (OsO4), with PBS wash steps in between. This was followed by serial dehydration in ethanol and hexamethyldisilazane (HMDS). The samples were coated with carbon and viewed with a Zeiss MERLIN FE-SEM with the InLens detector at 1kV. All SEM images (3 images per clot) were analysed using ImageJ where fibrin fibre width was assessed for each image using a grid overlay to accurately record these measurements. The central fibres in 12 squares on each image were measured.
Purified fibrinogen with LPS and RgpA
Purified fibrinogen (CoaChrom) was incubated with the following substances and prepared in technical triplicate following the above protocol, with the exception of using 0.15 U·mL-1 alpha-thrombin (CoaChrom, HF2A) to create the clots. Samples were viewed as above.
- RgpA at 20 µg·L-1
- LPS from gingivalis at 5 ng·L-1, 20 ng·L-1, and 20 µg·L-1
- LPS from coli O111:B4 at 5 ng·L-1, 20 ng·L-1, and 20 µg·L-1
- Combination of RgpA (20 µg·L-1) and LPS gingivalis (20 µg·L-1)
Confocal Microscopy on PPP with LPS
Platelet poor plasma was exposed to LPS from P. gingivalis (n=10; 10 ng·L-1; 30 min) and clotted with thrombin (7 U·mL-1; South African National Blood Service) on a microscope slide to create a fibrin fibre clot. Exposed clots were compared to their matched naïve samples by visualising intrinsic fluorescence on a Zeiss LSM 780 confocal microscope with a Plan-Apochromat 63x/1.4 oil DIC M27 objective using. Clot samples were excited by the 488nm laser with emission detected between 508-570nm and by the 561nm laser with emission detected between 593-700nm using. These settings were chosen after scanning the samples with the hyperspectral mode of the confocal with each laser and determining the best emission range for autofluorescent signal in these samples. The area coverage of the autofluorescent signal in the confocal images was analysed using ImageJ, with differences in the autofluorescent signal taken to reflect differences in the structure of the clot. Thresholding between 26 and 255 on the greyscale provided a consistent analysis of the images (3 images per clot). The percentage fluorescent area to total area of each image was compared between control and LPS‑exposed groups.
Confocal Microscopy with Airyscan on Fluorescent Fibrinogen with LPS
Fluorescently labelled Alexa Fluor™ 488 purified fibrinogen (2 mg·mL-1) was used to evaluate anomalous clotting, upon the addition of P. gingivalis LPS to the fibrinogen (100 ng·L-1; 30 min). Samples were clotted with thrombin (7 U·mL-1) on a microscope slide and viewed with the Zeiss MP880 confocal microscope in Airyscan mode. Exposed clots were compared to their matched naïve samples by exciting the fibrin fibres with the 488nm laser and collecting the emission with band pass filters 420-480nm and 495-550nm.
Confocal Microscopy on Fluorescent Fibrinogen with LPS
Fluorescently labelled Alexa Fluor™ 488 purified fibrinogen (2 mg·mL-1) was exposed to E. coli LPS (20 ng·L-1; 30 min; Sigma, L2630) or P. gingivalis LPS (20 ng·L-1; 30 min). Naïve and LPS-exposed samples were clotted with thrombin (7 U·mL-1) on a microscope slide and viewed on a Zeiss LSM 780 confocal microscope with a Plan-Apochromat 63x/1.4 oil DIC M27 objective. Images were captured in lambda mode with the 488nm laser and the GaAsP detector, which measures fluorescent emission between 410 and 695 nm across 32-channels, at 8.9 nm intervals. Multidimensional images were acquired as z-stacks and processed as maximum intensity projections in the ZEN software.
Correlative Atomic Force Microscopy and Raman Microspectroscopy on Fibrinogen with LPS
AFM-Raman was used to analyse the potential fibre structure changes in purified fibrinogen (Sigma) upon exposure to LPS from P. gingivalis (100 ng·L-1; 30 min). Purified fibrinogen was clotted on 10 mm gold‑coated coverslips (HORIBA Scientific, France) with thrombin (7 U·mL-1). Naïve clots were prepared with addition of thrombin. The glass coverslips were allowed to dry for about 2 minutes, before being submerged in PBS, followed by fixation in 4% formaldehyde and 1% osmium tetroxide, with PBS wash steps in between. Samples were dehydrated in increasing grades ethanol, before an ultimate HMDS drying step.
The characterisation of the samples was performed with a LabRAM Nano. This multi-analysis platform consists of a Raman microspectrometer (LabRAM HR Evolution, HORIBA) combined with an AFM (SmartSPM, HORIBA Scientific) for chemical and physical analysis of the same samples area. The system is based on a reflection configuration capable of approaching the objective lens (Mitutoyo, 100× magnification, NA=0.7, 20 mm working distance) from top illumination to the sample surface. Incident light is focused through the objective lens onto the apex of the AFM tip probe. In this study, micro-Raman images were measured with the 473nm laser as the excitation source (3mW maximum at the sample). Initially, three different wavelengths (473 nm, 532 nm and 633 nm) were tested. It was determined that the 473 nm was the best choice, and the Raman spectrum was measured in one window. The LabRAM Nano is equipped with an Edge filter to cut the Rayleigh signal so that the Stokes signal could be measured. Raman images were collected from 10µm2 regions with 0.3µm pixel steps. Acquisition time of each Raman spectrum is 30 seconds (one spectrum/image pixel). Correlated AFM images were obtained in AC mode using an ACCESS-NC Silicon probe (k = 25-95N/m, f = 200-400kHz, AppNano, US). The shape of the probes allows a direct visualisation of the tip apex, which permits correlation with the excitation Raman. AFM images were acquired from 20×10µm areas (300×150pts) for the control sample and 20×20µm areas (300×300pts) for the experimental sample.
Viscoelastic Analysis
The Thrombelastograph® (TEG®) 5000 Hemostasis Analyzer (Haemoscope Corp) was used to measure the viscoelastic properties of blood, with the measured parameters listed in Table 1. PPP samples were exposed to LPS from P. gingivalis (n=10; 10 ng·L-1; Sigma, SMB00610) or RgpA (n=30; 500 ng·L-1; Abcam, ab225548) for 30 minutes, with exposed samples compared to their matched naïve samples. Prepared PPP was placed in a TEG cup, together with 0.01M calcium chloride (CaCl2) to activate the coagulation process. The process was allowed to run until maximal amplitude (MA) was reached.
Table 1: TEG® parameters (modified from [56].
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Thromboplastic parameters
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Description
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R: Reaction time (minutes)
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Time of latency from start of test to initial fibrin formation (amplitude of 2 mm); i.e. initiation time
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α angle: (slope between the traces represented by R-time at 2mm and K-time at 20mm) (degrees)
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The angle measures the speed at which fibrin build up and cross linking takes place, hence assesses the rate of clot formation; i.e. thrombin burst
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MA: Maximal amplitude (mm)
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Maximum strength/stiffness of clot. Reflects the ultimate strength of the fibrin clot; i.e. overall stability of the clot
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MRTG: Maximum rate of thrombus generation (Dyn·cm-2·s-1)
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The maximum velocity of clot growth observed or maximum rate of thrombus generation using G, where G is the elastic modulus strength of the thrombus in dynes·cm-2
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TMRTG: Time to maximum rate of thrombus generation (minutes)
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The time interval observed before the maximum speed of the clot growth
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TTG: Total thrombus generation (Dyn·cm-2)
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The clot strength: the amount of total resistance (to movement of the cup and pin) generated during clot formation. This is the total area under the velocity curve during clot growth, representing the amount of clot strength generated during clot growth
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Rheometry of WB and PDP with LPS and RgpA
Whole blood (WB) (n=2) and PDP (n=2) were subjected to rheometry analysis on a Physica MCR 301 rheometer (Anton Paar, Austria) equipped with a Peltier controlled stainless steel sand-blasted cone-plate system (diameter 50 mm), mounted by a tempered hood and an evaporation blocker filled with silicon oil. The RheocompassTM software (v1.22, Anton Paar, Austria) was used for data acquisition.
Samples were prepared by exposing blood from control donors for 1 hour to either (1) LPS from E. coli (20 ng·L-1), (2) LPS from P. gingivalis (20 ng·L-1 or 20 µg·L-1) or (3) RgpA (100 ng·L-1 or 250 ng·L-1). Matching control runs were diluted with the same volume of vehicle as for the exposed samples. Experiments were run in technical triplicate.
Whole blood and plasma were clotted by addition of 0.01M CaCl2 and clots were generated in the cone-plate geometry. A constant sinusoidal strain amplitude (0.1 %, 1.5 Hz) was set to observe the process of clot formation with minimal interference. These time sweeps were conducted until a G’ plateau was reached, at which point an amplitude sweep test was started. The amplitude sweep tests were stress‑controlled with a logarithmic ramp from 1 to 5000 Pa at constant frequency (1 rad s-1).
The rheometry parameters discussed in this paper are given in Table 2. During the amplitude sweep tests, we continuously monitored the resulting strain (γ) of the material, which is the response of the clot to the applied sinusoidal stress (τ). The shift of the phase angle (δ) allows the calculation of the storage modulus (G’) by multiplying the stress-strain relationship (τ/γ) with cos(δ). G’ serves as a measure of the reversibly stored and thus recoverable deformation energy and represents clot stiffness. As long as G’ is maintained while the shear stress increases, the clot remains in its linear viscoelastic range (in its equilibrium) and experiences only elastic deformation. The clot can return into its initial form when the sinusoidal stress input crosses the 0-point. This can be also seen in the output waveform signal, which remains sinusoidal. With the continuous increase of shear force, a deviation from the initial G’ value and a change in the output waveform signal occurs, which marks the onset of the non-linear response. From this shear stress onwards, the clot cannot return into its initial equilibrium state since the stronger deformation does not allow full recovery. The borderline between the linear and the non-linear behaviour marks the elastic limit of the clot. As stresses become higher, non-linearity increases until the clot breaks. Since G’ can be a misleading measure of the elastic modulus of plastically deforming clots, because other harmonic components may also store energy (see [58], we applied the model of Ewoldt and coworkers [59] integrated in the Rheocompass software to calculate clot compliance out of Bowditch-Lissajous plots using an approach that is geometrically motivated [60]. The minimum-strain compliance shown here (J’M) reflects the tangent modulus at zero instantaneous stress, whereas the large-strain compliance (J’L) reflects the secant modulus at maximum stress (Figure 1). At equilibrium (linear clot behaviour), both compliances merge, whereas out of equilibrium they diverge (non-linear behaviour). Certain points on the curves indicate certain processes in the network, e.g., fibre bending and stretching out network inhomogeneities at intermediate shear stresses, stretching of the clot as a whole in shear direction at higher shear stresses, and weakening or even breaking of network points prior to complete breakup at highest-most shear stresses. Figure 1 shows these suggested regions. We propose that not only an upshift or downshift of the curves – indicating higher or lower compliances – must be considered to classify clots, but also changes in the shape of the compliance curves as they indicate specific clot behaviours. For example, the stress needed to fully stretch out the clot as a whole indicates the end of microscopic processes within the fibre network. Only if all branch points and inhomogeneities are aligned to the force lines, the clot stretches as a whole, which is referred to as macroscopic shear stiffening.