Dimensionless mean velocity, comparison

A comparison of the dimensionless mean velocity between the results experimentally measured and calculated is shown in Fig. 1.11 while that of the dimensionless intensity in Fig. 1.12. Note that the calculation based on the theoretical model requires a value for an adjustable parameter. From the figures, it seems that the agreement between the calculated values and the experimentally measured data is excellent. In addition. Fig. 1.12 provides the information of significance below the intensity of the axial component exceeds that of the radial component. 

Figure 4.7 Comparison of the profiles of dimensionless mean velocity versus dimensionless depth for 4> = 24° and V = 11.5,18.0,23.5. The solid lines are the numerical solution of the full equations the dots are the approximate algebraic solution.

Fig. 22.9 Comparison of the dimensionless mean drop size depending on the relative velocity of the gas phase. The drop size is predicted sufficiently by the prediction for completely filled capillaries. The same tendencies as for the threads emerging from completely filled capillaries are evident, as the drop size increases slightly with the gas-Weber ntmiber and higher flow rate originates larger drops. The viscosity has minor irrfluence on the mean drop size...

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