この研究は、静磁界が単一酵母細胞の出芽に及ぼす影響を、強い磁界(2.93T)および磁場勾配(6100 T2/ m)を発生できる磁気回路を用いて調査した。酵母細胞サッカロマイセス・セレヴィシエを、一様または非一様な静磁界下において、シリカ製毛細管(1辺0.1mmの角形管)入れた含水YPD寒天培地で増殖させた。その結果、4時間の磁界ばく露では、出芽酵母細胞の大きさに対する磁界影響はわずかであったが、出芽角度に対しては明らかな影響が見られた;均質磁界の場合、娘酵母細胞の出芽方向は主に磁界方向であった;不均質磁界の場合、娘酵母細胞は磁場勾配が高い方の領域にある毛細管流の軸に沿って出芽する傾向があった、と報告している。
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To evaluate the effect of static magnetic fields on the budding of single yeast cells.
Yeast cells were exposed in the center of a static magnetic field or in the inner or outer region of an inhomogeneous magnetic field.
Budding in yeast cells is a form of asexual reproduction. This process results in a mother and a smaller daughter cell.
ばく露 | パラメータ |
---|---|
ばく露1:
ばく露時間:
continuous for 4 hours
homogenous static magentic field
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|
ばく露2:
ばく露時間:
continuous for 4 hours
inhomogenous static magentic field
|
|
ばく露3:
ばく露時間:
continuous for 4 hours
inhomogenous static magentic field
|
|
The growth of yeast cells was monitored at three regions (the center, outside, and edge of the pole pieces), each with a width of 500 µm.
周波数 |
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タイプ |
|
ばく露時間 | continuous for 4 hours |
Additional information | homogenous static magentic field |
ばく露の発生源/構造 |
|
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チャンバの詳細 | yeast cells were exposed in a square fused-silica capillary in an agar solution that had a 100 x 100 mm² inner section, 300 x 300 mm² outer section, and was 7.5 cm in length; after setting, the capillaries were immediately subjected to the magnetic field experiments, which were conducted under dark conditions at 28.4±0.9 °C |
ばく露装置の詳細 | magnetic circuit (3 x 4 x 5 cm³) was constructed using two NdFeB magnets, two yokes, two pole pieces, four spacers and two frames; in the center of the magnetic circuit, a pair of iron pole pieces was set with a 400 or 600 µm-gap in a 4 x 4 mm² area; yeast was exposed in the center of the pole pieces |
Sham exposure | A sham exposure was conducted. |
測定量 | 値 | 種別 | Method | Mass | 備考 |
---|---|---|---|---|---|
磁束密度 | 2.93 T | maximum | 計算値 | - | at the center of the pole pieces |
周波数 |
|
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タイプ |
|
ばく露時間 | continuous for 4 hours |
Additional information | inhomogenous static magentic field |
ばく露の発生源/構造 |
|
---|---|
ばく露装置の詳細 | yeast was exposed in the edge of the pole pieces |
Sham exposure | A sham exposure was conducted. |
測定量 | 値 | 種別 | Method | Mass | 備考 |
---|---|---|---|---|---|
参照 | - | - | - | - | magnetic gradient (B x (dB/dx)) of 6100 T²/m (maximum) at the edge of the pole pieces |
参照 | - | - | - | - | magnetic gradient of 1600 T²/m (minimum) at the edge of the pole pieces |
周波数 |
|
---|---|
タイプ |
|
ばく露時間 | continuous for 4 hours |
Additional information | inhomogenous static magentic field |
ばく露の発生源/構造 |
|
---|---|
ばく露装置の詳細 | yeast was exposed outside of the pole pieces |
Sham exposure | A sham exposure was conducted. |
測定量 | 値 | 種別 | Method | Mass | 備考 |
---|---|---|---|---|---|
参照 | - | - | - | - | magnetic gradient (B x (dB/dx)) of 6100 T²/m (maximum) at the edge of the pole pieces |
参照 | - | - | - | - | magnetic gradient of 1600 T²/m (minimum) at the edge of the pole pieces |
After exposure to one of the different magnetic field conditions, the growth of budding yeast cells was slightly inhibited compared to unexposed cells. However, the magnetic field exposure clearly influenced the budding angle. After exposure to a homogeneous magnetic field the budding direction of daughter cells was mainly oriented in the direction of the magnetic field. In the inhomogeneous magnetic field, the daughter cells tended to bud along the axis where the magnetic gradient was high. No differences in the budding angle were seen between the inner and outer region of the inhomogeneous field.
The authors conclude that the direction of the magnetic field was the main factor controlling the budding direction of yeast cells.
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