strain transformation
Let be a Euclidean plane. Fix a line in and a real number . Take any point . Drop a line from perpendicular to . Denote the distance from to . Then there is a unique point on such that
The function such that is called a strain transformation, or simply a strain.
One can visualize a strain stretches a geometric figure if and compresses it if . If , then is the identity function, the only time when a strain is a rigid motion. For example, let be the -axis and be a circle in the upper half plane of the - plane. Then the following diagrams show how a strain transforms :
Again, if is the -axis, then is the function that sends to . Representing the ordered pairs as column vectors and as a matrix , we have
Nevertheless, a strain, as a (non-singular) linear transformation, takes lines to lines, and parallel lines to parallel lines.
In general, given any finite dimensional vector space over a field , a strain is a non-singular diagonalizable linear transformation on such that leaves a subspace of codimension fixed. is called the strain coefficient.
Remark. By choosing an appropriate base for of dimension , can be represented as a diagonal matrix whose diagonals are in at least cells and in at most one cell.
It is easy to see that every non-singular diagonalizable linear transformation on can be written as a product of strains, where .
Title | strain transformation |
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Canonical name | StrainTransformation |
Date of creation | 2013-03-22 17:25:45 |
Last modified on | 2013-03-22 17:25:45 |
Owner | CWoo (3771) |
Last modified by | CWoo (3771) |
Numerical id | 5 |
Author | CWoo (3771) |
Entry type | Definition |
Classification | msc 15A04 |
Synonym | strain |
Defines | strain coefficient |