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ANNUAL REPORT - MTA SzFKI

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Fig. 1. ns-EC to s-EC transition induced (a) by increase of the temperature T (polarizing microscopy); (b) by<br />

increase of the voltage U (light diffraction fringes). n denotes the initial director.<br />

Interactions at liquid crystal surfaces. — Experiments on director gliding have been<br />

carried out on Arabic gum and glucose layers. On Arabic gum flow alignment has been<br />

detected with permanent director orientation, while on glucose layers gliding has been<br />

found, which has speeded up above the glass-transition temperature of the glucose (32 o C).<br />

According to the first measurements, the distribution of relaxation times of the gliding<br />

process is much narrower for glucose than on corresponding polymer layers.<br />

Granular flow. — The flow properties of a granular layer of thickness h on an inclined<br />

plane (inclination angle θ) can be characterized by the so called flow rule, which describes<br />

the thickness dependence of the surface velocity u. The flow rule of granular flows on a<br />

rough inclined plane has been measured for various materials, including sand and glass<br />

beads of various sizes and four types of copper particles with different shapes. The<br />

materials have been characterized by measuring h s , the thickness at which the flow stops,<br />

as a function of the plane inclination on various surfaces. Measuring the surface velocity u<br />

of the gravity induced flow as a function of the flow thickness h, deviations from the<br />

Pouliquen flow rule u/(gh) 0.5 ~h/h s have been detected for sand and glass beads. An<br />

improved collapse of the experimental data has been obtained by using a recently proposed<br />

scaling of the form u/(gh) 0.5 =β htan 2 θ/h s tan 2 θ 1 where θ 1 is the angle at which the h s curves<br />

diverge. Measuring the slope β for ten different sizes of sand and glass beads, we find a<br />

systematic, strong increase of β with the divergence angle θ 1 . Copper materials with<br />

different shapes could not well be described by either flow rule.<br />

E-Mail:<br />

Tamás Börzsönyi btamas@szfki.hu<br />

Ágnes Buka ab@szfki.hu<br />

Nándor Éber eber@szfki.hu<br />

Katalin Fodor-Csorba fodor@szfki.hu<br />

István Jánossy janossy@szfki.hu<br />

Tibor Tóth-Katona katona@szfki.hu<br />

Anikó Vajda vajda@szfki.hu<br />

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