Morton number
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: In fluid dynamics, the Morton number (Mo) is a
dimensionless number A dimensionless quantity (also known as a bare quantity, pure quantity, or scalar quantity as well as quantity of dimension one) is a quantity to which no physical dimension is assigned, with a corresponding SI unit of measurement of one (or 1) ...
used together with the Eötvös number or Bond number to characterize the shape of bubbles or drops moving in a surrounding fluid or continuous phase, ''c''. It is named after Rose Morton, who described it with W. L. Haberman in 1953.


Definition

The Morton number is defined as : \mathrm = \frac, where ''g'' is the acceleration of gravity, \mu_c is the
viscosity The viscosity of a fluid is a measure of its resistance to deformation at a given rate. For liquids, it corresponds to the informal concept of "thickness": for example, syrup has a higher viscosity than water. Viscosity quantifies the inte ...
of the surrounding fluid, \rho_c the
density Density (volumetric mass density or specific mass) is the substance's mass per unit of volume. The symbol most often used for density is ''ρ'' (the lower case Greek letter rho), although the Latin letter ''D'' can also be used. Mathematical ...
of the surrounding fluid, \Delta \rho the difference in density of the phases, and \sigma is the surface tension coefficient. For the case of a bubble with a negligible inner density the Morton number can be simplified to :\mathrm = \frac.


Relation to other parameters

The Morton number can also be expressed by using a combination of the Weber number, Froude number and Reynolds number, :\mathrm = \frac. The Froude number in the above expression is defined as :\mathrm = \frac where ''V'' is a reference velocity and ''d'' is the equivalent diameter of the drop or bubble.


References

{{NonDimFluMech Dimensionless numbers Bubbles (physics) Dimensionless numbers of fluid mechanics Fluid dynamics