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, Une fois que le premier minimum est atteint, l'intensité croît alors des images d à f le long de la branche d'interférence (2), ce qui correspond à un épaississement du film. Puis, à mesure que l'on se déplace en direction du ménisque avant (i.e. le long de l'axe x pour y = 0), l'intensité décroît en Fig. G.1.a. Cette variation correspond à une décroissance de l'intensité en direction du côté droit de la branche (1), caractérisant une augmentation de l'épaisseur du film. Une analyse similaire est effectuée pour chaque image
, Contrairement à la variation monotone de l'intensité dans le ménisque avant, un motif en forme de croissant est présent à l'arrière de la goutte (voir Fig. G.1.a), où l'intensité lumineuse varie sur toute la gamme de niveaux de gris. Ceci rend l'identification de l'épaisseur, a priori ambiguë
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