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U - Scientific Bulletin

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150 Christian Russu<br />

distributions found on the symmetry plane are represented against values<br />

calculated via analytical, one-dimensional model (figs. 5 & 6). It can be observed<br />

that the maximum values decrease as B/L ratio becomes smaller, going down to<br />

50% from the value calculated analytically, as the point where this value is<br />

achieved moves toward the trailing edge.<br />

Normalized pressure distribution<br />

Normalized pressure distribution<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

Analytical<br />

onedimensional<br />

B/L=1<br />

B/L=0.5<br />

B/L=2<br />

0 0.2 0.4 0.6 0.8 1<br />

Dimensionless coordinates x/L<br />

Fig. 5. Pressure distribution in median section.<br />

Rayleigh step model. Analytical vs. numerical.<br />

Analytical<br />

onedimensional<br />

B/L=2<br />

B/L=1<br />

B/L=0.5<br />

0 0.2 0.4 0.6 0.8 1<br />

Dimensionless coordinates x/L<br />

Fig. 6. Pressure distribution in median section.<br />

Convergent gap model. Analytical vs. numerical.<br />

For the spherical model, we have a convergent zone of the contact<br />

followed by a divergent one. This limits the real active area as shown in fig. 7. It

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