この研究は、C57b雄マウスの皮下に植え付けたB16-BL6メラノーマ細胞の成長に対する低レベル磁界の影響を調べた。ばく露に用いたのはThomasパターン(15ms幅の2峰ピーク波が規則的に断続するようなパターン)をもつ磁界であり、発生方法は、1)面状ソレノイドコイルによる不均一磁界(中心で5μT);2)ヘルムホルツコイルによる均一磁界(5μT);3)2個の対向コイルによる打ち消し合った磁界(地磁気レベル5-15μT);4)2個の対向コイルに最も近い空間の強い磁界(2-5μT);5)2個の対向コイルから最も離れた空間の弱い磁界(1-5nT);6)3軸ソレノイドコイルによる空間回転磁界(2-5μT)の6条件と、擬似ばく露とケージコントロールである。その結果、特定の空間時間的構成となるよう調整された電磁界は、マウスの移植実験腫瘍の成長に影響する可能性があることが示されたと報告している。
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To measure the effect of exposure to a specific spatial-temporal electromagnetic field presented using different geometric configurations on the growth of experimental tumors in mice.
A total of 65 male mice were used. The experiment was performed in two separate blocks separated by six months to control for potential effects of the endogenous geomagnetic field: Block 1 contained 32 mice and block 2 contained 33 mice. Beginning on the day of cancer cell injection, the mice were exposed to two control (sham exposure and cage control) and six different magnetic field configurations (six groups of four mice) between 21 h and midnight (3 h) every day for 38 days.
ばく露 | パラメータ |
---|---|
ばく露1:
25 Hz
Modulation type:
pulsed
ばく露時間:
3 hr/day on 38 days
cylindrical field
|
|
ばく露2:
25 Hz
Modulation type:
pulsed
ばく露時間:
3 hr/day on 38 days
Helmholtz coils
|
|
ばく露3:
25 Hz
Modulation type:
pulsed
ばく露時間:
3 hr/day on 38 days
attenuated geomagnetic field
|
|
ばく露4:
25 Hz
Modulation type:
pulsed
ばく露時間:
3 hr/day on 38 days
low intensity field
|
|
ばく露5:
25 Hz
Modulation type:
pulsed
ばく露時間:
3 hr/day on 38 days
high intensity field
|
|
ばく露6:
25 Hz
Modulation type:
pulsed
ばく露時間:
3 hr/day on 38 days
rotating field
|
周波数 | 25 Hz |
---|---|
タイプ |
|
ばく露時間 | 3 hr/day on 38 days |
Additional information | cylindrical field |
Modulation type | pulsed |
---|---|
Additional information |
Thomas pattern, for further information see Thomas et al. 1997 |
ばく露の発生源/構造 | |
---|---|
ばく露装置の詳細 | two 25 cm x 1 cm solenoids created by 1050 turns of insulated wire wound around an iron nail; solenoids separated by 20 cm: mice placed in 20 cm x 30 cm x 20 cm plastic cages in the heterogenous field between the solenoids |
Sham exposure | A sham exposure was conducted. |
測定量 | 値 | 種別 | Method | Mass | 備考 |
---|---|---|---|---|---|
磁束密度 | 5 µT | - | 測定値 | - | at the central axis |
周波数 | 25 Hz |
---|---|
タイプ |
|
ばく露時間 | 3 hr/day on 38 days |
Additional information | Helmholtz coils |
Modulation type | pulsed |
---|---|
Additional information |
Thomas pattern, for further information see Thomas et al. 1997 |
ばく露の発生源/構造 | |
---|---|
ばく露装置の詳細 | two Helmholtz coils 30 cm apart; each constructed by wrapping a 39 cm x 39 cm box with 305 m of 3 American Wire Gauge in a single layer, 18 cm wide ; mice placed in 20 cm x 30 cm x 20 cm plastic cages in the homogenous field between the coils |
Sham exposure | A sham exposure was conducted. |
測定量 | 値 | 種別 | Method | Mass | 備考 |
---|---|---|---|---|---|
磁束密度 | 5 µT | - | 測定値 | - | - |
周波数 | 25 Hz |
---|---|
タイプ |
|
ばく露時間 | 3 hr/day on 38 days |
Additional information | attenuated geomagnetic field |
Modulation type | pulsed |
---|---|
Additional information |
Thomas pattern, for further information see Thomas et al. 1997 |
ばく露の発生源/構造 | |
---|---|
ばく露装置の詳細 | two opposing double Helmholtz coils created by wrapping two 112 cm x 125 cm plastic boxes with 72 turns of 30 AWG wire in a single layer, 13 cm wide; coils placed 2 cm apart; two stainless steel shelfs for shielding of the geomagnetic field |
Sham exposure | A sham exposure was conducted. |
周波数 | 25 Hz |
---|---|
タイプ |
|
ばく露時間 | 3 hr/day on 38 days |
Additional information | low intensity field |
Modulation type | pulsed |
---|---|
Additional information |
Thomas pattern, for further information see Thomas et al. 1997 |
ばく露の発生源/構造 |
|
---|---|
ばく露装置の詳細 | adjacent housing area furthest from the activated coil used |
Sham exposure | A sham exposure was conducted. |
周波数 | 25 Hz |
---|---|
タイプ |
|
ばく露時間 | 3 hr/day on 38 days |
Additional information | high intensity field |
Modulation type | pulsed |
---|---|
Additional information |
Thomas pattern, for further information see Thomas et al. 1997 |
ばく露の発生源/構造 |
|
---|---|
ばく露装置の詳細 | housing area nearest to the activated coil used |
Sham exposure | A sham exposure was conducted. |
周波数 | 25 Hz |
---|---|
タイプ |
|
ばく露時間 | 3 hr/day on 38 days |
Additional information | rotating field |
Modulation type | pulsed |
---|---|
Additional information |
Thomas pattern, for further information see Thomas et al. 1997 field for 0.5 s in each opposing solenoid within the X-, Y-, Z-plane, then for 0.5 s in all planes simultaneously |
ばく露の発生源/構造 | |
---|---|
ばく露装置の詳細 | three pairs of solenoids; each solenoid placed in the center of each face of a 30 cm x 30 cm x 30 cm cube; |
Sham exposure | A sham exposure was conducted. |
Mice exposed to the field that was rotated through the three spatial dimensions and through all three planes every two seconds (see field 6) did not grow tumors after 38 days. However, the animals in the sham exposed field and cage controls showed massive tumors after 38 days. Tumor growth was also affected by the intensity of the field, with mice exposed to a weak intensity field (1-5 nT, field 4) forming smaller tumors than animals exposed to sham exposure or high intensity (2-5 µT) fields. The mice exposed to the cylindrical field, Helmholtz field, attenuated geomagnetic field, high intensity field, or the sham exposure conditions formed large tumours that were not different from the non-handled cage controls.
Immunohistochemistry of tumors from those mice exposed to the different intensity fields suggested that alterations in leukocyte infiltration or vascularization could contribute to the differences in tumor growth.
The authors conclude that exposure to specific spatial-temporal regulated electromagnetic field configurations had potent effects on the growth of experimental tumors in mice. These effects were also dependent on the intensity and special complexity of the field pattern.
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