Abstract
In many gas-solid flow studies it has to be considered that the particle phase may not move with a uniform one-dimensional velocity, but may show at any place of measuring a particular velocity distribution the mean of which may be distinctly different from the fluid’s local mean velocity. Generally this happens with particle sizes exceeding the order of a few microns and because of the turbulence of the fluid flow. The character of those distributions may rarely be assessed theoretically. The complete frequency distributions of the local particle velocities therefore have to be determined by registering the velocities of individual particles passing through an exactly limited probe volume.
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