Rotem and Shinnar [7] derived numerical solutions for the
one-dimensional flow of power-law fluids.
The second example under investigation is the transient modeling of
one-dimensional flow in a homogenous unsaturated inclined slope.
They solved the fundamental equations of mass, momentum, and energy assuming
one-dimensional flow. They followed this paper with a second publication (El Moueddeb et al.
Following a simplified model by Plas [1], consider an idealized
one-dimensional flow entering a BLI jet engine at [u.sub.1], and leaving the engine nozzle at [u.sub.2].
Swaroop and Mehta [2] have obtained a solution to the problem of
one-dimensional flow in unsaturated porous media taking finite element approach.
The dashed curves correspond to the
one-dimensional flow and the solid ones to the two-dimensional flow.
His topics include optoisolation
one-dimensional flow and bifurcation, optoisolation negative differential resistance circuits as a dynamical system, optoisolation circuit two-dimensional flow, optoisolation circuit time period delay differential equation, and optoisolation circuit chaos characteristics.
For
one-dimensional flow of perfect gas without any energy loss, the ideal pressure rise for given diffuser can be computed by considering energy conservation.
The truncated power-law model, in which the power-law model is terminated at the limiting Newtonian viscosities, has been applied to this situation without sacrificing the power-law equations for
one-dimensional flow [5, 10, 11].
Soon centrifugal impeller design using
one-dimensional flow theory became routine.