In classical gases, this quantity follows the Maxwell-Boltzmann distribution, which assumes that each component of this vector is normally distributed.
The pressure gradient is defined as viscosity times the Laplacian of this quantity in creeping flow. In classical gases, the most probable magnitude of this quantity is equal to two-thirds of the root mean square magnitude of this quantity. The curl of this quantity for a fluid is the (*) vorticity. In classical gases, this quantity follows the Maxwell-Boltzmann distribution, which assumes that each component of this vector is normally distributed. For 10 points, name this vector quantity whose addition in special relativity ensures it can never exceed that of light, the time derivative of the position vector.
The pressure gradient is defined as viscosity times the Laplacian of this quantity in creeping flow.
{velocity}