Terminal Velocity of Falling Particles

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This Demonstration calculates the terminal velocity of a spherical solid particle falling in a fluid under the force of gravity.

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Three forces act on the particle: the downward force of gravity, an upward force of buoyancy, and a drag force that acts opposite to the direction of motion of the particle. The equation relating these forces to the particle acceleration is:

,

where is the radius of the sphere; and are the densities of the fluid and the particle, respectively; is the gravitational constant; is the particle velocity; and is the drag coefficient that varies with the Reynolds number, , as follows [1]:

,

where is the viscosity in and is the particle diameter; CGS units are used throughout. The equation for is valid over the entire range of the available experimental data; use beyond is not reliable. For the equation follows the creeping flow result . You can calculate the terminal velocity, the Reynolds number, and the drag coefficient over a wide range of the variables , , , , and . The artificial values of gravity included in the calculation can be achieved particularly in space, but also on Earth.

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Contributed by: Clay Gruesbeck (June 2015)
Open content licensed under CC BY-NC-SA


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Reference

[1] F. A. Morrison, “Data Correlation for Drag Coefficient for Sphere,” Department of Chemical Engineering, Michigan Technological University, 2013. http://www.chem.mtu.edu/~fmorriso/DataCorrelationForSphereDrag2013.pdf.



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