Fig. 2.
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Total magnetic flux evolution for three chosen ARs and corresponding fits with the three-segment broken lines. The segments are fitted from the first frame until the maximum magnetic flux. The first broken point was chosen as a representative time for the beginning of the steep increase of the magnetic flux and therefore as the moment that the emergence starts (it corresponds to the normalised time T = 0). The time of reaching the flux maximum corresponds to the normalised time T = 1.
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