For an ideal gas, this quantity is proportional to temperature raised to the three-halves power divided by temperature plus a constant. This quantity jumps from zero to non-zero when entering the boundary layer. In substances where it is only a function of temperature, the shear stress is equal to this quantity times the first derivative of the velocity profile with respect to a change in position perpendicular to the direction of shear. The velocity times a characteristic length divided by the kinematic form of this quantity equals the Reynolds number. Newtonian fluids have constant value of, for 10 points, what measure of a fluid's resistance to flow?
For an ideal gas, this quantity is proportional to temperature raised to the three-halves power divided by temperature plus a constant. This quantity jumps from zero to non-zero when entering the boundary layer. In substances where it is only a function of temperature, the shear stress is equal to this quantity times the first derivative of the velocity profile with respect to a change in position perpendicular to the direction of shear. The velocity times a characteristic length divided by the kinematic form of this quantity equals the Reynolds number. Newtonian fluids have constant value of, for 10 points, what measure of a fluid's resistance to flow?
For an ideal gas, this quantity is proportional to temperature raised to the three-halves power divided by temperature plus a constant.
viscosity [accept dynamic viscosity until "kinematic," do not accept "kinematic viscosity"]