This study introduces an experiment designed to analyze the sensorimotor adaptation to a motion-based sound synthesis system. We investigated a sound-oriented learning task, namely to reproduce a targeted sound. The motion of a small handheld object was used to control a sound synthesizer. The object angular velocity was measured by a gyroscope and transmitted in real time wirelessly to the sou...

In conventional near-field acoustic holography (NAH) it is not possible to distinguish between sound from the two sides of the array, thus, it is a requirement that all the sources are confined to only one side and radiate into a free field. When this requirement cannot be fulfilled, sound field separation techniques make it possible to distinguish between outgoing and incoming waves from the t...

Sound velocity and attenuation in liquid sulfur have been measured at temperatures from 80 °C in the super cooled state through the melting temperature ~about 120 °C! to 200 °C under saturated pressure. The measurements were performed with a pulsed phase sensitive technique at frequencies from 5 to 22 MHz. Accuracy of the sound velocity measurements was 0.1%. A distinct feature in sound velocit...

The dependence of some thermodynamic properties of spin-polarized liquid 3He such as velocity of sound, adiabatic index, isentropic compressibility and temperature on the spin polarization has been investigated along different isentropic paths. The Lennard-Jones potential has been used in our calculations. It has been found that for higher values of entropy, the spin polarization has greate...

Formulas are presented for an incompressible inviscid velocity field V with a vorticity field Ω outside of a rigid sphere and for the far-field sound generation. The velocity V is expressed as the sum of an image velocity v∗ and a known velocity v in <3, which is induced by the same vorticity field Ω outside the sphere and the extension Ω = 0 inside. We derive formulas for the image velocity v∗...