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In the context of particulate motion the Péclet number has also been called Brenner number, with symbol Br, in honour of Howard Brenner. [ 2 ] The Péclet number also finds applications beyond transport phenomena, as a general measure for the relative importance of the random fluctuations and of the systematic average behavior in mesoscopic ...
Dimensionless numbers (or characteristic numbers) have an important role in analyzing the behavior of fluids and their flow as well as in other transport phenomena. [1] They include the Reynolds and the Mach numbers, which describe as ratios the relative magnitude of fluid and physical system characteristics, such as density, viscosity, speed of sound, and flow speed.
Basic reproduction number: number of infections caused on average by an infectious individual over entire infectious period: epidemiology: Body fat percentage: total mass of fat divided by total body mass, multiplied by 100: biology Kt/V: Kt/V: medicine (hemodialysis and peritoneal dialysis treatment; dimensionless time) Waist–hip ratio
It is a dimensionless number, closely related to the fluid's Rayleigh number. [1]: 466 A Nusselt number of order one represents heat transfer by pure conduction. [1]: 336 A value between one and 10 is characteristic of slug flow or laminar flow. [2]
In fluid mechanics, the Rayleigh number (Ra, after Lord Rayleigh [1]) for a fluid is a dimensionless number associated with buoyancy-driven flow, also known as free (or natural) convection. [2] [3] [4] It characterises the fluid's flow regime: [5] a value in a certain lower range denotes laminar flow; a value in a higher range, turbulent flow.
Fig 2: The grid used for discretisation in Upwind Difference Scheme for positive Peclet number (Pe>0) Fig 3: The grid used for discretisation in Upwind Difference Scheme for negative Peclet number (Pe < 0) By putting these values in equation and rearranging we get the following result,
[1] [2] [3] The effect is named after the British fluid dynamicist G. I. Taylor, who described the shear-induced dispersion for large Peclet numbers. The analysis was later generalized by Rutherford Aris for arbitrary values of the Peclet number. The dispersion process is sometimes also referred to as the Taylor-Aris dispersion.
The number is named after Italian scientist Carlo Marangoni, although its use dates from the 1950s [1] [2] and it was neither discovered nor used by Carlo Marangoni. The Marangoni number for a simple liquid of viscosity μ {\displaystyle \mu } with a surface tension change Δ γ {\displaystyle \Delta \gamma } over a distance L {\displaystyle L ...