| Literature DB >> 33020513 |
Xabier Murgia1,2, Andreas M Kany3,4, Christian Herr5, Duy-Khiet Ho1, Chiara De Rossi1, Robert Bals5, Claus-Michael Lehr1,6, Anna K H Hirsch3,4,6, Rolf W Hartmann3,4,6, Martin Empting7,8,9, Teresa Röhrig10,11.
Abstract
Lung infections caused by Pseudomonas aeruginosa pose a serious threat to patients suffering from, among others, cystic fibrosis, chronic obstructive pulmonary disease, or bronchiectasis, often leading to life-threatening complications. The establishment of a chronic infection is substantially related to communication between bacteria via quorum-sensing networks. In this study, we aimed to assess the role of quorum-sensing signaling molecules of the Pseudomonas quinolone signal (PQS) and to investigate the viscoelastic properties of lung tissue homogenates of PA-infected mice in a prolonged acute murine infection model. Therefore, a murine infection model was successfully established via intra-tracheal infection with alginate-supplemented Pseudomonas aeruginosa NH57388A. Rheological properties of lung homogenates were analyzed with multiple particle tracking (MPT) and quorum-sensing molecules were quantified with LC-MS/MS. Statistical analysis of bacterial load and quorum-sensing molecules showed a strong correlation between these biomarkers in infected lungs. This was accompanied by noticeable changes in the consistency of lung homogenates with increasing infection severity. Furthermore, viscoelastic properties of the lung homogenates strongly correlated with bacterial load and quorum sensing molecules. Considering the strong correlation between the viscoelasticity of lung homogenates and the aforementioned biomarkers, the viscoelastic properties of infected lungs might serve as reliable new biomarker for the evaluation of the severity of P. aeruginosa infections in murine models.Entities:
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Year: 2020 PMID: 33020513 PMCID: PMC7536435 DOI: 10.1038/s41598-020-73459-5
Source DB: PubMed Journal: Sci Rep ISSN: 2045-2322 Impact factor: 4.379
Figure 1Dependence of signal molecule production on bacterial load. (a) Scatterplot and linear regression of the quorum sensing signaling molecules PQS (2-heptyl-3-hydroxy-4(1H)-quinolone) vs HHQ (2-heptyl-4-quinolone) detected in murine Pseudomonas aeruginosa NH57388A lung infection samples. (b,c) Scatterplot and linear regression of PQS (B) and HHQ (C) vs corresponding colony forming units (CFU). See also Fig. S1.
Figure 3Rheological properties strongly correlate with bacterial biomarkers. Scatterplot and linear regression of colony forming units (CFU; a), PQS (b) and HHQ (c) vs tracer particle logMSD (logarithm of mean square displacement at τ = 0.1 s) and exponential coefficient α. See also Fig. S4.
Figure 2Representative mean squared displacement (MSD) plots as a function of the time scale (τ) of polyethylene glycol-coated polystyrene particles. (a–c) mean squared displacement (MSD) of each individual tracer particle trajectory at different τ in representative lung homogenates of murine Pseudomonas aeruginosa NH57388A lung infection samples. All animals were infected with the same bacterial inoculum but developed different degrees of infection that correlated with low (a), medium (b), and high (c) viscoelasticity. The mean and the median of all individual particles are indicated by the red and blue lines, respectively. (d–f) corresponding distribution of the logMSD at a τ = 0.1 s. See also Fig. S2. Tracer particles had a mean diameter of 218 nm. (g–i) Representative mean squared displacement (MSD) distributions at τ = 0.108 s normalized by the ensemble-average MSD (〈MSD) at τ = 0.108 s. See also Fig. S3.
Summary of multiple particle tracking (MPT) analysis of each lung homogenate from 12 independent mice.
| 〈MSD | D | α | η | G0 | ||
|---|---|---|---|---|---|---|
| [µm2] | [µm2/s] | [mPa*s] | [Pa] | [nm] | ||
| Mouse #1 | 0.368 ± 0.12 | 0.901 ± 0.26 | 0.94 ± 0.11 | 2.41 ± 0.75 | a | a |
| Mouse #2 | 0.376 ± 0.10 | 0.891 ± 0.22 | 0.93 ± 0.11 | 2.41 ± 0.88 | a | a |
| Mouse #3 | 0.348 ± 0.10 | 0.828 ± 0.21 | 0.91 + 0.12 | 2.60 ± 0.85 | a | a |
| Mouse #4 | 0.228 ± 0.16 | 0.764 ± 0.23 | 0.73 ± 0.34 | 3.03 ± 1.99 | 1.57 ± 1.07 | 157 ± 52 |
| Mouse #5 | 0.161 ± 0.17 | 0.794 ± 0.29 | 0.61 ± 0.31 | 3.05 ± 1.9 | 0.75 ± 0.59 | 208 ± 72 |
| Mouse #6 | 0.277 ± 0.16 | 0.746 ± 0.35 | 0.79 ± 0.22 | 3.32 ± 1.58 | a | a |
| Mouse #7 | 0.182 ± 0.16 | 0.673 ± 0.33 | 0.72 ± 0.32 | 4.23 ± 3.60 | 1.56 ± 0.90 | 146 ± 24 |
| Mouse #8 | 0.057 ± 0.09 | 0.520 ± 0.22 | 0.34 ± 0.31 | 5.03 ± 3.07 | 1.16 ± 1.01 | 179 ± 59 |
| Mouse #9 | 0.086 ± 0.11 | 0.512 ± 0.24 | 0.47 ± 0.35 | 6.22 ± 6.03 | 1.75 ± 1.40 | 160 ± 54 |
| Mouse #10 | 0.004 ± 0.005 | b | 0.11 ± 0.10 | b | 3.03 ± 1.51 | 118 ± 24 |
| Mouse #11 | 0.006 ± 0.005 | b | 0.20 ± 0.17 | b | 2.84 ± 1.67 | 123 ± 27 |
| Mouse #12 | 0.006 ± 0.010 | b | 0.13 ± 0.12 | b | 2.48 ± 1.21 | 129 ± 39 |
〈MSD, ensemble-averaged mean squared displacement from all trajectories; D diffusion; α exponential coefficient; η viscosity; G plateau modulus; ξ mess size. D and η were average from all trajectories with α > 0.8, whereas Go and ξ were averaged from trajectories with α < 0.2.
aNot enough trajectories (less than 10) with α < 0.2 to compute G0 and ξ.
bNot enough trajectories (less than 10) with α > 0.8 to compute D and η. Mean ± Standard deviation are shown.