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Powell–Eyring Stress Terms

Mathematical Modelling — Fluid Dynamics & Heat TransferContinuum mechanics; boundary-layer similarity theory

LT⁻²

Symbol

The shear-thinning viscous diffusion and nonlinear retardation stresses that make the fluid non-Newtonian.

Main equation
Level 0 of 9
Brief — named quantities
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Dimension:LT⁻² (m s⁻²)Maths:ℝ scalar(·, ·, ·) — A single number (real numbers), depending on another quantity, another quantity, another quantityDimensionally verifiedMathematically verifiedFully reduced to base quantities

In words:minus.

Equation Workspace

Set known values, calculate unknowns, inspect dependencies, and run numerical solves.

Calculator

Equation workspace

Set the values you know, then calculate the remaining quantities in Powell–Eyring Stress Terms.

Domain Analysis

Unit status, dimensional trails, per-step checks, and custom unit expressions.

Try your own — the unit calculator

Ever wondered whether a formula “adds up”? This tool answers one plain question: do the units match? Pick a couple of quantities (distance, time, a speed…), join them with ×, ÷, +, or =, and press Run. It works out the resulting unit — for example distance ÷ time gives a speed, LT⁻¹ (metres per second) — and flags anything that can’t be right, like adding a length to a time.

Reads as: τ

“τ” is analysed by expanding its full defining equation (its children and their relations), not as a bare symbol. Use Check this concept’s units above for the same result.

Mathematical Analysis

Object type, lawful operations, conditions, comparisons, and derivation-step checks.

Equation

Dimension I

Definition

What it is — and what it is not

What it is
  • S1The non-Newtonian stress contribution of the Powell–Eyring model in the momentum equation.
Wisdoms
  • S2It encodes shear-thinning: apparent viscosity falls as the shear rate rises.
Attributes
  • S3A linear viscous diffusion plus a nonlinear retardation.

Dimension II

In practice

How to deal with it

No practical guidance recorded yet.

Sub-topics 2

Prerequisite

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