A Newtonian fluid’s shear stress is directly proportional to the rate of shear strain. This linear relationship is defined by Newton’s law of viscosity: \(\tau = \mu \frac{du}{dy}\), where \(\tau\) is the shear stress, \(\mu\) is the dynamic viscosity (a constant of proportionality), and \(\frac{du}{dy}\) is the shear rate or velocity gradient.
