Ohnesorge number

The Ohnesorge number (Oh) is a dimensionless number that relates the viscous forces to inertial and surface tension forces. The number was defined by Wolfgang von Ohnesorge in his 1936 doctoral thesis.^{[1] [2]}

It is defined as:

${\displaystyle \mathrm {Oh} ={\frac {\mu }{\sqrt {\rho ,円\sigma ,円L}}}={\frac {\sqrt {\mathrm {We} }}{\mathrm {Re} }}\sim {\frac {\mbox{viscous forces}}{\sqrt {{\mbox{inertia}}\cdot {\mbox{surface tension}}}}}}${\displaystyle \mathrm {Oh} ={\frac {\mu }{\sqrt {\rho ,円\sigma ,円L}}}={\frac {\sqrt {\mathrm {We} }}{\mathrm {Re} }}\sim {\frac {\mbox{viscous forces}}{\sqrt {{\mbox{inertia}}\cdot {\mbox{surface tension}}}}}}

Where

• μ is the dynamic viscosity of the liquid
• ρ is the density of the liquid
• σ is the surface tension
• L is the characteristic length scale (typically drop diameter)
• Re is the Reynolds number
• We is the Weber number

The Ohnesorge number for a 3 mm diameter rain drop is typically ~0.002. Larger Ohnesorge numbers indicate a greater influence of the viscosity.

This is often used to relate to free surface fluid dynamics such as dispersion of liquids in gases and in spray technology.^{[3] [4]}

In inkjet printing, liquids whose Ohnesorge number are in the range 0.1 < Oh < 1.0 are jettable (1<Z<10 where Z is the reciprocal of the Ohnesorge number).^{[1] [5]}

• Laplace number - There is an inverse relationship, ${\displaystyle \mathrm {Oh} =1/{\sqrt {\mathrm {La} }}}${\displaystyle \mathrm {Oh} =1/{\sqrt {\mathrm {La} }}}, between the Laplace number and the Ohnesorge number. It is more historically correct to use the Ohnesorge number, but often mathematically neater to use the Laplace number.

• Dimensionless numbers of fluid mechanics
• Fluid dynamics
• Fluid dynamics stubs

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