| Literature DB >> 12069691 |
Paul A Harris1, Justin Lamb, Brian Heaton, Denys N Wheatley.
Abstract
BACKGROUND: The issue remains unresolved as to whether low frequency magnetic fields can affect cell behaviour, with the possibility that they may be in part responsible for the increased incidence of leukaemia in parts of the population exposed to them.Entities:
Year: 2002 PMID: 12069691 PMCID: PMC116433 DOI: 10.1186/1475-2867-2-3
Source DB: PubMed Journal: Cancer Cell Int ISSN: 1475-2867 Impact factor: 5.722
Figure 1A : Magnetic field distribution in the vertical plane; (- - - - -) represents the boundary of the ± 2.5% cylindrical uniform magnetic field; (- - -) represents the boundary of the sample holder. B: Magnetic field distribution in the horizontal plane demonstrating cylindrical symmetry; (- - - -) represents the boundary of the ± 2.5% cylindrical uniform magnetic field; (- - -) represents the boundary of the sample holder.
Figure 2Flow cytometry histograms of synchronised HeLa S3 cells. From left to right the histograms correspond to 7.5, 9, 10.5, 11.5 and 13 h after release of the second thymidine block. Categories 3 and 4 have been irradiated with a dose of 1 Gy in early S-phase.
Figure 8Flow cytometry histograms of synchronised HeLa S3 cells corresponding to categories 3 and 4. Each row corresponds to cultures irradiated with 5 Gy and assessed for nuclear DNA content approximately 13 h after release of the second thymidine block.
Statistics applied to flow cytometry data
| 1 & 2 | 0 | Wilcoxon matched pairs | 22 | ns |
| 3 & 4 | 1 | " | 13 | 0.05 |
| 3 & 4 | 3 | " | 25 | 0.01 |
| 3 & 4 | 5 | " | 8 | 0.05 |
| 3 & 4 | 5 | Student's t-test | 4 | 0.05 |
| 3 & 4 | 1, 3 & 5 | Wilcoxon matched pairs | 20 | 0.01 |
Perpendicular components of background time-varying and static magnetic fields measured at location of sample holders
| Component of System | Active (Yes/No) | Time-Varying Field | Static Field |
| coils A,B | no | 3nT | 50.3 μT |
| coils C,D | no | 3nT | 45.6 μT |
| Amplifier and Signal Generator | no | ||
| coils A,B | no | 3nT | |
| coils C,D | no | 3nT | |
| Amplifier and Signal Generator | yes | ||
| coils A,B | yes | 2mT* | |
| coils C,D | no | 0.38 μT* | |
| Amplifier and Signal Generator | yes |
* With alternate Helmholtz pairs active the background time-varying field in the non-active coils was found to be 0.38 μT.