We present arguments in support of the view that Newton’s first law of motion extends itself to stochastic motions as follows: Every entity perseveres in its state of independent and stationary increments except insofar as it is compelled to change its state by forces impressed. Some of the ...
As a result, for such near-wall simple shear flow, the equation of motion (15) takes the form: −𝑑𝑝𝑑𝑥+𝜌𝜒𝑛𝑑𝑑𝑦[𝜈𝑑𝑢2𝑛−1𝑑𝑦]1𝑛=0.−dpdx+ρχnddyνdu2n−1dy1n=0. (16) In the case of negative 𝑑𝑢𝑑𝑦dudy after expanding...