However there are few reports on validation of the

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Unformatted text preview: S.l nom (1) ) − d 1 + d 2 .v M (1) ⎪ Fy(1) = 0 ⎨ ⎪ Fz(1) = 0 ⎪ ⎩ In this example, we realise that pair positions have an influence on boundary conditions applied on the component, in particular on seal forces values. By the same way, actual geometric deviation modify distance between the 2 components hence the boundary conditions values. Our model takes into account this influence. These vector form deviation noted (uF(i), vF(i), wF(i)) can be found in equations associated to the mechanism. Figure 7: Actual geometry deviations and there influence on boundary conditions If we consider component 1 actual geometry deviation, we can write equations expressing this influence: d1 Fx (1) = S .( Lini - lnom (1) − .v M (1) - v F (1) ) d1 + d 2 with ∆x[1] given by experimentation, for example: vF(1)= 0,5 S .d 1 Fx (1) = S .( Lini - lnom (1) - 0,5) − .v M (1) d1 + d 2 forces ⎤ ⎡ Where Fx(1) belongs to ⎢ ⎥ matrix and vΜ(1) belongs to [V] matrix. ⎣displacement ⎦ Once establis...
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This note was uploaded on 08/03/2010 for the course DD 1234 taught by Professor Zczxc during the Spring '10 term at Magnolia Bible.

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