The Newton's law for viscosity
where "F" - force, has the dimension "[{\\rm{LM}}{{\\rm{T}}^{ - 2}}]", "A" - area of contact, hast the dimension "[{{\\rm{L}}^2}]" and "{{\\partial v} \\over {\\partial x}}" - velocity gradient has the dimension "{\\rm{[}}{{\\rm{T}}^{ - 1}}]" (because "v" has the dimension "[{\\rm{L}}{{\\rm{T}}^{ - 1}}]" and "x" has the dimension "[{\\rm{L}}]" ). Let "\\eta" has the dimension "[X]". Then, using the Newton's law for viscosity
Thus
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