| Literature DB >> 30609680 |
Alexandra N Hurst1,2,3, Beth Scarbrough4,5,6, Roa Saleh7, Jessica Hovey8, Farideh Ari9, Shreya Goyal10,11, Richard J Chi12,13, Jerry M Troutman14,15,16, Juan L Vivero-Escoto17,18,19.
Abstract
Photodynamic inactivation (PDI) is a non-antibiotic option for the treatment of infectious diseases. Although Gram-positive bacteria have been shown to be highly susceptible to PDI, the inactivation of Gram-negative bacteria has been more challenging due to the impermeability properties of the outer membrane. In the present study, a series of photosensitizers which contain one to four positive charges (1⁻4) were used to evaluate the charge influence on the PDI of a Gram-negative bacteria, Escherichia coli (E. coli), and their interaction with the cell membrane. The dose-response PDI results confirm the relevance of the number of positive charges on the porphyrin molecule in the PDI of E. coli. The difference between the Hill coefficients of cationic porphyrins with 1⁻3 positive charges and the tetra-cationic porphyrin (4) revealed potential variations in their mechanism of inactivation. Fluorescent live-cell microscopy studies showed that cationic porphyrins with 1⁻3 positive charges bind to the cell membrane of E. coli, but are not internalized. On the contrary, the tetra-cationic porphyrin (4) permeates through the membrane of the cells. The contrast in the interaction of cationic porphyrins with E. coli confirmed that they followed different mechanisms of inactivation. This work helps to have a better understanding of the structure-activity relationship in the efficiency of the PDI process of cationic porphyrins against Gram-negative bacteria.Entities:
Keywords: E. coli; cationic porphyrin; gram-negative bacteria; photodynamic inactivation
Mesh:
Substances:
Year: 2019 PMID: 30609680 PMCID: PMC6337135 DOI: 10.3390/ijms20010134
Source DB: PubMed Journal: Int J Mol Sci ISSN: 1422-0067 Impact factor: 5.923
Figure 1Chemical structure of the porphyrins used in this work. Four cationic porphyrin derivatives were synthesized: 1–4 with one to four positive charges, respectively. Compound 2 is a mixture of the cis and trans isomer. 5 and 6 are commercially available and used as control compounds.
Figure 2(A) Normalized absorption and (B) emission spectra for 10 µM solutions of 1 (blue), 2 (red), 3 (black) and 4 (orange) in DMSO. The four Q absorption bands are shown in the inset.
Photophysical parameters for cationic porphyrins including extinction coefficient values (ε), fluorescence (ΦF) and 1O2 (ΦΔ) quantum yields.
| Porphyrin | λSoret (nm) | λEmission (nm) a | ΦF (520 nm) b | ΦΔ
c |
|---|---|---|---|---|
|
| 418 [355 ± 22] | 649, 716 | 0.11 ± 0.01 | 0.65 ± 0.04 |
|
| 418 [285 ± 19] | 649, 715 | 0.10 ± 0.01 | 0.61 ± 0.03 |
|
| 418 [248 ± 30] | 648, 715 | 0.12 ± 0.01 | 0.61 ± 0.06 |
|
| 418 [324 ± 38] | 647, 713 | 0.11 ± 0.01 | 0.65 ± 0.04 |
a λex = 520 nm. b Fluorescence quantum yields in DMSO were calculated based on the fluorescence spectra using TPP (Benzene) as a standard (ΦF = 0.12) [14]; λex = 520 nm. c 1O2 quantum yields in DMF were calculated using TPP (DMF) as a standard (ΦΔ = 0.62) [21]; λIrradiation = 515 nm.
Figure 3Time-dependent plots for the decay of DMA photosensitized by 1 (blue), 2 (red), 3 (black), 4 (orange), 5 (purple) and TPP (brown) in DMF at irradiation wavelength of 515 nm. Values include the mean and standard deviation of three independent experiments.
Figure 4Bacterial toxicity with 1 (blue), 2 (red), 3 (black), 4 (orange), 5 (purple) and 6 (green) against E. coli in the absence of light (top) and after light exposure for 20 min (bottom). E. coli was incubated with cationic porphyrin derivatives for 30 min. Minimal dark toxicity was observed at concentrations below 1 µM. Values represent the average of three independent experiments. Error bars represent one standard of deviation. Statistical analysis was performed by one-way ANOVA (**** p < 0.0001).
Analysis of PDI efficiency using the EC50 and EC99.99 parameters. Values for EC50 were determined by best fit analysis of a dose response curve on data from at least three independent experiments, with additional experiments using concentrations at or near the initial EC50 value for refinement. Hill coefficients were determined by analysis of log plots and adjusted incrementally for the best fit to the higher concentrations that did not result in complete inactivation. EC99.99 values were calculated from the EC50 and Hill coefficient with error propagation from the EC50 measurement. Error in the EC50 represents one standard of deviation from the fit mean value. All data for these measurements is provided in Figure S1.
| Porphyrin | EC50 (nM) | EC99.99 (nM) | Hill |
|---|---|---|---|
|
| 146 ± 13 | 5810 ± 520 | 2.5 |
|
| 10.7 ± 1.4 | 425 ± 56 | 2.5 |
|
| 1.3 ± 0.3 | 51 ± 11 | 2.5 |
|
| 11.4 ± 0.6 | 52.9 ± 2.8 | 6.0 |
|
| 29.0 ± 3.2 | 290 ± 32 | 4.0 |
Figure 5Micrographs depicting the interaction of cationic porphyrins with E. coli. 3 (top row) and 4 (bottom row). Left: Differential interference contrast image, middle: fluorescence image (medial z slice), and right: merge image. [PS] = 1 µM; Incubation time: 30 min.
Figure 6Micrographs of cationic porphyrin 4 with E. coli at various incubation times. (A) 5, (B) 10, (C) 15, and (D) 20 min. Left: Differential interference contrast image, middle: fluorescence image (medial z slice), and right: merge image. [PS] = 1 µM.
Figure 7Trend of cellular interaction between cationic porphyrins 3 (black) and 4 (orange) and E. coli cells as a function of increasing concentration of Mg+2 ions, source MgCl2 (0, 10, 25, 50 mM). The percentage of PS attached was calculated as a percentage of the original PS concentration (1 µM). Values represent the average of three independent experiments. Error bars represent one standard of deviation. Statistical analysis was performed by one-way ANOVA (* p < 0.05).