| Literature DB >> 29038998 |
Zsolt Bodai1, Simon Cameron2, Frances Bolt2, Daniel Simon3, Richard Schaffer3, Tamas Karancsi3, Julia Balog3, Tony Rickards2,4, Adam Burke2, Kate Hardiman2, Julia Abda2, Monica Rebec4, Zoltan Takats2.
Abstract
The recently developed automated, high-throughput monopolar REIMS platform is suited for the identification of clinically important microorganisms. Although already comparable to the previously reported bipolar forceps method, optimization of the geometry of monopolar electrodes, at the heart of the system, holds the most scope for further improvements to be made. For this, sharp tip and round shaped electrodes were optimized to maximize species-level classification accuracy. Following optimization of the distance between the sample contact point and tube inlet with the sharp tip electrodes, the overall cross-validation accuracy improved from 77% to 93% in negative and from 33% to 63% in positive ion detection modes, compared with the original 4 mm distance electrode. As an alternative geometry, round tube shaped electrodes were developed. Geometry optimization of these included hole size, number, and position, which were also required to prevent plate pick-up due to vacuum formation. Additional features, namely a metal "X"-shaped insert and a pin in the middle were included to increase the contact surface with a microbial biomass to maximize aerosol production. Following optimization, cross-validation scores showed improvement in classification accuracy from 77% to 93% in negative and from 33% to 91% in positive ion detection modes. Supervised models were also built, and after the leave 20% out cross-validation, the overall classification accuracy was 98.5% in negative and 99% in positive ion detection modes. This suggests that the new generation of monopolar REIMS electrodes could provide substantially improved species level identification accuracies in both polarity detection modes. Graphical abstract.Entities:
Keywords: Bacterial identification; Electrode geometry optimization; Monopolar electrod; REIMS; Rapid evaporative ionization mass spectrometry
Mesh:
Year: 2017 PMID: 29038998 PMCID: PMC5785610 DOI: 10.1007/s13361-017-1818-5
Source DB: PubMed Journal: J Am Soc Mass Spectrom ISSN: 1044-0305 Impact factor: 3.109
Figure 1Rapid evaporative ionization mass spectrometry (REIMS) setup with monopolar electrode for bacteria identification (a) and a CAD draw of the sharp electrode (b)
Figure 2Optimization workflow to decide which electrode gave the highest classification accuracy. Round shaped electrodes were optimized in separate batches; then the best electrodes were tested on the same bacteria colonies for final decision
Detailed Information of the Tested Electrodes
| ID | Shape | Hole on the wall of the electrode | Insert (diameter of pin/mm or width of X/mm) | Heating power (W) | PCA classification accuracy (%) | ||||
|---|---|---|---|---|---|---|---|---|---|
| Closest distance from the contact surface /mm | Shape | Number | Size (diameter/mm or width x height/mm) | Negative ion mode | Positive ion mode | ||||
| Original a | sharp | no holes | no holes | no holes | no holes | no insert | 17 | 77/80/87 | 33 |
| 3 mm b | sharp | no holes | no holes | no holes | no holes | no insert | 17 | 82 | 42 |
| 2 mm b | sharp | no holes | no holes | no holes | no holes | no insert | 17 | 93 | 61 |
| 1 mm b | sharp | no holes | no holes | no holes | no holes | no insert | 17 | 89 | 63 |
| 0.5 mm b | sharp | no holes | no holes | no holes | no holes | no insert | 17 | 90 | 49 |
| EL1 | round | 0.5 mm | circle | 5 | 1 | no insert | 40 | 86 | 60.5 |
| EL2 | round | 0.5 | circle | 3 | 1 | no insert | 40 | 92.5/90.5 | 66.5/91 |
| EL3 | round | 0.5 | circle | 3 | 1.5 | no insert | 40 | 86.5 | 52 |
| EL4 | round | 2.5 | circle | 3 | 1 | no insert | 40 | 91 | 52 |
| EL5 | round | 0 | half circle | 6 | 1 | no insert | 50 | 92/89 | 76.5/77 |
| N1 | round | 0 | rectangle | 4 | 0.5 × 0.5 | no insert | 50 | 83 | 78.5 |
| N2 | round | 0 | rectangle | 4 | 1 × 0.5 | no insert | 50 | 83 | 76.5 |
| N3 | round | 0 | rectangle | 4 | 0.5 × 1 | no insert | 50 | 84.5/93 | 80/85.5 |
| N4 | round | 0 | rectangle | 4 | 1 × 1 | no insert | 50 | 86 | 76.5 |
| X1 | round | 0.5 | circle | 2 | 1 | 0.25 X | 50 | 81.5 | 83 |
| X2 | round | 0.5 | circle | 2 | 1 | 0.5 X | 50 | 87/93.5 | 80.5/89 |
| X3 c | round | no holes | no holes | no holes | no holes | 0.5 X | 30 | 83 | 59.5 |
| XB | round | 0.5 | circle | 2 | 1 | 0.5 pin | 50 | 83.5 | 74.5 |
| X4 | round | 0.5 | circle | 2 | 1 | 1 X | 80 | 88 | 82.5 |
| X5 | round | 0.5 | circle | 2 | 1 | 2X | 110 | 77 | 58.5 |
| XC1 | round | 0 | rectangle | 4 | 0.5 × 0.5 | 1 X | 100 | 86.5 | 84 |
| XC2 | round | 0 | rectangle | 4 | 0.5 × 0.5 | 2X | 110 | 79.5 | 72 |
aDistance between the contact point and the entrance to electrode tubing is 4 mm.
bDistance between the contact point and the entrance to electrode tubing.
cThe cross was raised 0.1 mm from the pa.
Figure 3Signal-to-noise ratio with different heating power in the case of Streptococcus pneumoniae with EL5 in negative ion detection mode. Optimal heating powers were selected for the heating power that gave the maximum signal-to-noise or where a plateau had been reached
Figure 4Classification accuracy results in negative and positive ion mode with different distance between the contact point and inlet to the sharp electrode probe. Long distance resulted in less precise classification accuracy
Figure 5Classification accuracy results in negative and positive ion mode with different diameter of X insert inside the electrode. Increased contact surface also meant smaller inlet space, thus, aspiration of analyte containing vapor was less effective and classification accuracy was lower