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Even in this case, the box is still much wider (in x) than the thickness of the SP layer, S P / L ∼ S - 1 / 2 ∼ 3 10 - 4, and much longer (in y) than L c / L ∼ S c / S ∼ 10 - 3
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Even in this case, the box is still much wider (in x) than the thickness of the SP layer, S P / L ∼ S-1 / 2 ∼ 3 10-4, and much longer (in y) than L c / L ∼ S c / S ∼ 10-3.
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When a typical plasmoid is ejected from its host layer into a bigger plasmoid, it is long and thin: w x ∼ w y E eff (Ref. 13). However, immediately upon ejection, it is squashed against the bigger plasmoid and becomes circularized (w x ∼ w y), while preserving its flux and area. Thus, just before it starts coalescing with the bigger plasmoid, its width jumps uby a factor of E eff - 1 / 2 ∼ 10, and its magnetic field becomes B 0 E eff 1 / 2 to preserve flux. This immediately moves the plasmoid vertically upwards by a factor E eff - 1 / 2 from the ULS diagonal. Our arguments can be modified to account for this effect-the result is to raise the threshold (2) upwards by a factor of order unity
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When a typical plasmoid is ejected from its host layer into a bigger plasmoid, it is long and thin: w x ∼ w y E eff (Ref. 13). However, immediately upon ejection, it is squashed against the bigger plasmoid and becomes circularized (w x ∼ w y), while preserving its flux and area. Thus, just before it starts coalescing with the bigger plasmoid, its width jumps up by a factor of E eff-1 / 2 ∼ 10, and its magnetic field becomes B 0 E eff 1 / 2 to preserve flux. This immediately moves the plasmoid vertically upwards by a factor E eff-1 / 2 from the ULS diagonal. Our arguments can be modified to account for this effect-the result is to raise the threshold (2) upwards by a factor of order unity.
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