Physics · Glossary

What is Newtonian viscosity?

Definition 4.1 University Physics — Year 2 · Chapter 4 — Viscous Flows

In a plane shear flow v=vx(y)ex\vect v = v_x(y)\,\vect e_x, the fluid above a surface y=y = const exerts on the fluid below it (through a surface element  ⁣dS\dd S) the tangential force

 ⁣dF=η ⁣dvx ⁣dy ⁣dS  ex,\dd\vect F = \eta\,\frac{\dd v_x}{\dd y}\,\dd S\;\vect e_x ,

dragging the slower layer forward and being dragged back in return. The shear stress is τ=η ⁣dvx/ ⁣dy\tau = \eta\,\dd v_x/\dd y; the coefficient η\eta (unit Pas\mathrm{Pa}\,\mathrm{s}) is the dynamic viscosity of the fluid, and ν=η/ρ\nu = \eta/\rho (m2/s\mathrm{m}^{2}/\mathrm{s}) its kinematic viscosity. A fluid for which η\eta does not depend on the shear rate is Newtonian: water, air, oils, alcohol; blood, paint, ketchup and polymer melts are not. Orders of magnitude at 20C20{}^{\circ}\mathrm{C}: air η=1.8×105Pas\eta = 1.8 \times 10^{-5}\,\mathrm{Pa}\,\mathrm{s} (ν=1.5×105m2/s\nu = 1.5 \times 10^{-5}\,\mathrm{m}^{2}/\mathrm{s}), water 1.0×103Pas1.0 \times 10^{-3}\,\mathrm{Pa}\,\mathrm{s} (ν=1.0×106m2/s\nu = 1.0 \times 10^{-6}\,\mathrm{m}^{2}/\mathrm{s}), olive oil 0.08Pas0.08\,\mathrm{Pa}\,\mathrm{s}, glycerol 1.5Pas1.5\,\mathrm{Pa}\,\mathrm{s}, honey 10Pas\sim10\,\mathrm{Pa}\,\mathrm{s}. Liquids get thinner when heated, gases thicker.

Left: plane Couette flow between a fixed plate and a plate moving at U — a linear profile, the same shear stress on every layer. Right: the viscous forces on a slab of fluid; they cancel unless the velocity profile is curved.
Left: plane Couette flow between a fixed plate and a plate moving at UU — a linear profile, the same shear stress on every layer. Right: the viscous forces on a slab of fluid; they cancel unless the velocity profile is curved.

Examples

Example 4.4 (Shear stress on a table)

A 0.1mm0.1\,\mathrm{mm} film of oil (η=0.1Pas\eta = 0.1\,\mathrm{Pa}\,\mathrm{s}) between a plate and a table, the plate sliding at 1m/s1\,\mathrm{m}/\mathrm{s}: τ=ηU/h=1kPa\tau = \eta U/h = 1\,\mathrm{kPa}, a force of 100N100\,\mathrm{N} on a tenth of a square metre — the principle of the lubricated bearing, where the viscous drag replaces dry friction a hundred times larger. Honey on a spoon, 10Pas10\,\mathrm{Pa}\,\mathrm{s}, 1mm1\,\mathrm{mm} thick, draining at 1mm/s1\,\mathrm{mm}/\mathrm{s}: τ=10Pa\tau = 10\,\mathrm{Pa}, exactly the weight of a millimetre of honey per unit area — which is why it drains at that speed.

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