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Bodenstein number

The Bodenstein number is a dimensionless parameter in chemical reaction engineering, which describes the ratio of the amount of substance introduced by convection to that introduced by diffusion. Hence, it characterises the backmixing in a system and allows statements whether and how much volume elements or substances within a chemical reactor mix due to the prevalent currents. It is defined as the ratio of the convection current to the dispersion current. The Bodenstein number is an element of the dispersion model of residence times and is therefore also called the dimensionless dispersion coefficient.

Determination of the Bodenstein number
The Bodenstein number is calculated according to :\mathit{Bo}=\frac{u \cdot L}{D_\mathrm{ax}} where • u: flow velocity • L: length of the reactor • D_\mathrm{ax}: axial dispersion coefficient It can also be determined experimentally from the distribution of the residence times. Assuming an open system: :\sigma_\theta^2=\frac{\sigma^2}{\tau^2}=\frac{2}{\mathit{Bo}}+\frac{8}{\mathit{Bo}^2} holds, where • \sigma^{2}_{\theta}: dimensionless variance • \sigma^2: variance of the mean residence time • \tau: hydrodynamic residence time The Bodenstein number is similar to the Péclet number, which is applied in thermodynamics and in fluid mechanics. The axial dispersion coefficient correlates with the axial Péclet number. \mathit{Pe_{ax}}=\frac{u \cdot \widetilde{L}}{D_{ax}} where • \widetilde{L}: – characteristic length \mathit{Bo}=\mathit{Pe_{ax}}\cdot\frac{\widetilde{L}}{L} == References ==
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