. Le-miroir-unique-n, est pas parfaitement parallèle à la face de sortie de la calcite. Par ailleurs, si l'incidence du faisceau source sur la face d'entrée de cette dernière n'est pas rigoureusement normale, il peut exister une petite différence de marche géométrique

L. Raideur-associée-À-ce-ménisque, avec ? ? 25 mN.m ?1 la tension de surface de l'hexadécane à 35 ° C et rm ? 1 mm le rayon de courbure du ménisque), est quant à elle bien trop faible

. La-pression-minimale and . Qu, il est possible d'atteindre dans notre machine à dépôts est de 3.10 ?7 mbar environ, mais il faut pour cela réaliser un pompage de près de 14 heures. 4. On protège alors les pompes en les isolant de l'enceinte à l

P. Fabriqué-en, ordre de 4 GPa ?, il pourra être remplacé par un équivalent plus rigide, fabriqué par exemple en Dural ? matériau de module d'Young de 75 GPa ?, si l'on cherche à maximiser davantage la raideur K de la machine Du côté de la sphère, une contribution à cette raideur machine peut provenir de la torsion du joint de flexion autour de l'axe vertical des efforts sphère-plan. En effet, malgré une raideur en torsion très élevée ? de l'ordre de 2.10 6 N.m.rad ?1 ? le mouvement de l'extrémité libre du joint de flexion portant le miroir de mesure peut comporter une petite composante en rotation induisant une erreur sur le déplacement mesuré. L'asymétrie inévitable de la sphère

S. Dans-le and . De-lyon, une telle rotation du bilame servant à la mesure de force explique d'ailleurs pourquoi la raideur machine mesurée est plus faible en configuration "immergée" dans laquelle le plan est déporté (cf. photographie 3.5 droite), le bras de levier entre le point d'application des forces sur le plan et l'axe de torsion du bilame étant alors bien plus grand qu'en configuration "goutte". Les effets de serrage et de positionnement des surfaces sur leurs supports, ainsi que l'asymétrie, jamais reproductible, de la sphère expliquent la légère variabilité de la raideur machine mesurée d'une campagne d'expériences SFA à l'autre

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