---
title: "Generalised Hooke's law for isotropic materials"
subject: "Mechanics of Solids"
chapter: 4
key: "semester_5/mechanics_of_solids:generalised-hooke-law-isotropic"
source: https://www.bctengineer.com/q/semester_5/mechanics_of_solids/generalised-hooke-law-isotropic
site: BCT Engineering
---

# Generalised Hooke's law for isotropic materials

Mechanics of Solids · Chapter 4: General Hooke’s Law

- Asked in: year not given, 6 marks
- Video: [08.4 Generalized Hooke's Law](https://www.youtube.com/watch?v=UDMNrUt-0cE) — Introductory Engineering Mechanics
- Answer checked by Claude Sonnet 5.5 on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_5/mechanics_of_solids/generalised-hooke-law-isotropic
- Whole chapter: https://www.bctengineer.com/md/semester_5/mechanics_of_solids/chapter-4

## Question

State the generalised Hooke's law. Write the stress-strain relations for a linear isotropic material, define the elastic constants $E$, $G$, $\nu$ and $K$ and show the relations between them. How many independent constants are needed for anisotropic, orthotropic and isotropic materials?

## Short answer

Generalized Hooke’s law: σ_ij = C_ijkl ε_kl (21 independent constants for anisotropy). Isotropic form: ε_x = [σ_x-ν(σ_y+σ_z)]/E, γ_xy = τ_xy/G. Elastic constants: E (Young’s), ν (Poisson’s), G (shear), K (bulk). Relations: G = E/[2(1+ν)], K = E/[3(1-2ν)]. Two independent constants. Anisotropic: 21, orthotropic: 9, isotropic: 2.

## Answer

#### Generalised Hooke's law

For a linear elastic body each stress component is a linear function of all strain components:
$\sigma_{ij} = C_{ijkl}\,\varepsilon_{kl}$, where $C_{ijkl}$ is the elasticity (stiffness) tensor. Because $\sigma_{ij}$ and $\varepsilon_{ij}$ are symmetric and a strain energy function exists, the 81 constants reduce to **21** for the most general anisotropic body.

#### Isotropic material

$$
\begin{aligned}
\varepsilon_x &= \frac{1}{E}\left[\sigma_x - \nu(\sigma_y+\sigma_z)\right] &\qquad \gamma_{xy} &= \frac{\tau_{xy}}{G} \\
\varepsilon_y &= \frac{1}{E}\left[\sigma_y - \nu(\sigma_z+\sigma_x)\right] & \gamma_{yz} &= \frac{\tau_{yz}}{G} \\
\varepsilon_z &= \frac{1}{E}\left[\sigma_z - \nu(\sigma_x+\sigma_y)\right] & \gamma_{zx} &= \frac{\tau_{zx}}{G}
\end{aligned}
$$

Inverse (Lamé form): $\sigma_{ij} = \lambda\,\varepsilon_{kk}\delta_{ij} + 2G\varepsilon_{ij}$, with $\lambda = \dfrac{\nu E}{(1+\nu)(1-2\nu)}$.

#### Elastic constants

| Constant | Definition |
|---|---|
| Young's modulus $E$ | $\sigma/\varepsilon$ in uniaxial tension |
| Poisson's ratio $\nu$ | $-\varepsilon_{lateral}/\varepsilon_{axial}$ |
| Shear modulus $G$ | $\tau/\gamma$ in pure shear |
| Bulk modulus $K$ | $p/\varepsilon_v$ under hydrostatic pressure |

#### Relations

Adding the three normal strain equations gives the volumetric strain
$\varepsilon_v = \dfrac{1-2\nu}{E}(\sigma_x+\sigma_y+\sigma_z)$. For a hydrostatic pressure $p$ (taking the magnitude, with compression positive) the sum of the three stresses is $3p$ in magnitude, so

$$
K = \frac{p}{\varepsilon_v} = \frac{E}{3(1-2\nu)}
$$

Pure shear: the principal stresses are $\pm\tau$, so $\varepsilon_1 = \dfrac{\tau}{E}(1+\nu)$. Since $\gamma = 2\varepsilon_1$ (the principal axes are at $45^\circ$ to the shear planes) and $\gamma = \tau/G$,

$$
G = \frac{E}{2(1+\nu)}
$$

Hence $E = 9KG/(3K+G)$ and $\nu = (3K-2G)/(2(3K+G))$. Only **two** of the four constants are independent.

#### Number of independent constants

| Material | Independent constants |
|---|---|
| General anisotropic | 21 |
| Orthotropic (three perpendicular symmetry planes, e.g. timber) | 9 |
| Transversely isotropic | 5 |
| Isotropic | 2 |

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. What does the generalised Hooke's law state?
   A. Each stress component is a linear function of all strain components, via the stiffness tensor C_ijkl
   B. Stress equals strain squared
   C. Each stress depends only on its own strain
   D. Strain depends on stress rate
   Answer: A. sigma_ij = C_ijkl eps_kl, with 81 constants reducing to 21 for general anisotropy. (Key point: Generalised Hooke's law)

2. Which expression gives K?
   A. E/(2(1 + nu))
   B. E/(3(1 - 2nu))
   C. E/(1 - 2nu)
   D. 3E(1 - 2nu)
   Answer: B. From eps_v = (1 - 2nu) 3p / E, K = p/eps_v = E/(3(1 - 2nu)). (Key point: Bulk modulus)

3. How is G = E/(2(1+nu)) obtained?
   A. From hydrostatic pressure
   B. From uniaxial tension with eps_lateral
   C. From pure shear: principal stresses +/- tau, eps_1 = tau(1 + nu)/E, and gamma = 2 eps_1 = tau/G
   D. From the Lame constant only
   Answer: C. Pure shear is equivalent to principal stresses +/- tau, and gamma = 2 eps_1 at 45 degrees equals tau/G. (Key point: Shear modulus relation)

4. Which list of independent constants is correct (anisotropic, orthotropic, isotropic)?
   A. 9, 21, 2
   B. 21, 5, 2
   C. 21, 2, 9
   D. 21, 9, 2
   Answer: D. General anisotropic has 21, orthotropic 9, isotropic 2. (Key point: Number of constants)

## Related in Mechanics of Solids

- [Strain-displacement relations and strain tensor](https://www.bctengineer.com/question.md?key=semester_5%2Fmechanics_of_solids%3Astrain-displacement-small-displacement) — Mechanics of Solids, chapter 3
- [Strain energy density and thermal stress](https://www.bctengineer.com/question.md?key=semester_5%2Fmechanics_of_solids%3Astrain-energy-density-thermal-constraint) — Mechanics of Solids, chapter 4
- [Material response, isotropy and temperature effect](https://www.bctengineer.com/question.md?key=semester_5%2Fmechanics_of_solids%3Aelastic-response-isotropy-temperature) — Mechanics of Solids, chapter 1
- [Elastic-plastic torsion of a circular shaft](https://www.bctengineer.com/question.md?key=semester_5%2Fmechanics_of_solids%3Aplastic-torsion-circular-shaft) — Mechanics of Solids, chapter 12
- [Strain rosette: principal strains and stresses](https://www.bctengineer.com/question.md?key=semester_5%2Fmechanics_of_solids%3Astrain-rosette-principal-numerical) — Mechanics of Solids, chapter 3

## Related in other subjects

- [Isotropic vs anisotropic; Lame's constants](https://www.bctengineer.com/question.md?key=semester_8%2Fcomputational_techniques_in_civil_engineering%3Aisotropic-anisotropic-lame) — Computational Techniques in Civil Engineering, chapter 3
- [True stress and true strain relations](https://www.bctengineer.com/question.md?key=semester_3%2Fmaterial_science%3Atrue-stress-strain-relations) — Material Science, chapter 3
- [Stress-strain curves: linear and non-linear cases](https://www.bctengineer.com/question.md?key=semester_5%2Fconcrete_technology_and_masonry_structure%3Astress-strain-nonlinear-cases) — Concrete Technology and Masonry Structure, chapter 4
- [Stress-strain curve of ductile material](https://www.bctengineer.com/question.md?key=semester_3%2Fcivil_engineering_materials%3Astress-strain-curve-ductile) — Civil Engineering Materials, chapter 1
