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09 / CHAPTER 02

Deformation and displacement

Describe how a body changes shape in space.

Continuum Mechanics: original course diagram
A visual model for this course. Read it as a prompt for the assumptions behind the chapter.

ANCHOR EQUATION

Small strain

ε=12∇u+∇Tu

In symbols: ε = ½(∇u + ∇uᵀ)

The symmetric displacement gradient measures small deformation without rigid rotation.

Displacement maps material points

A solid or fluid element changes position and shape. A motion map labels a material point by its reference coordinate X and returns its current position x(X,t), separating identity from location.

Differentiate the motion map

Write x = χ(X,t). The deformation gradient F = ∂x/∂X tells how a small material vector dX becomes dx = F dX. Its determinant J = det F gives local volume ratio: J > 1 expansion, J < 1 compression. Velocity is ∂χ/∂t at fixed X.

If x = 2X in one dimension, a segment dX = 0.01 m becomes dx = 0.02 m; stretch ratio is 2. If x = X + 0.1tX, stretch grows as 1 + 0.1t.

Large rotations are not necessarily strain

A rigid body can rotate with F orthogonal and preserve lengths, so deformation measures must separate rotation from stretch. Treating displacement magnitude as strain confuses motion with shape change.

Work it: For 2D map x = 2X + Y, y = X + 2Y, form F, compute det F, and state whether area doubles, shrinks, or stays constant.