Reconstruct deformation without equating shape and stress
Strain describes a change in shape or size; stress describes force per area. A deformed marker can constrain a deformation history only if its original geometry and later preservation are independently justified. The same final shape does not uniquely identify the applied stress, temperature, strain rate or material response.
Learning outcome: Compare the original circle and transformed boundary. Calculate determinant, both stretches and ellipse area. Distinguish observed final shape from assumptions about the initial marker and from an unmeasured stress history.
Starting recap
Keep map geometry, relative displacement, source magnitude and conditional hazard evidence distinct. A model probability is not a deterministic forecast.
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At γ=1 and r=2, stretches are about 1.61803 and 0.618034, giving semiaxes 3.23607 and 1.23607. Their product remains r²=4, so ellipse area is 4π, equal to the original circle.
Open the experimentPredict
Can a rock marker become elongated without a change in area?
Experiment
Compare the original circle and transformed boundary. Calculate determinant, both stretches and ellipse area. Distinguish observed final shape from assumptions about the initial marker and from an unmeasured stress history.
Separate shape change, rotation and area conservation
Worked teaching model · synthetic values · Original 2-D deformation x′=x+γy, y′=y. Initial circle radius b; determinant is one, so area is conserved. Principal stretches are square roots of eigenvalues of FᵀF. Finite homogeneous shape comparison, not an elastic stress law or actual rock strain measurement.
Reset keeps your prediction, captures and practice history.
A marker can change shape substantially while preserving its area.
Simple shear combines shape change and rotation; principal stretches are not simply the diagonal entries of the deformation matrix. Stress, elastic recovery and brittle failure require material and loading information absent here.
| Quantity | Value | Unit |
|---|---|---|
| Deformation determinant | 1 | ratio |
| Original marker area | 12.5663706 | area units |
| Deformed marker area | 12.5663706 | area units |
| Maximum principal stretch | 1.61803399 | ratio |
| Minimum principal stretch | 0.618033989 | ratio |
| Principal semiaxis maximum | 3.23606798 | length units |
| Principal semiaxis minimum | 1.23606798 | length units |
| x | y |
|---|---|
| 2 | 0 |
| 2.2439421 | 0.26105238 |
| 2.4494897 | 0.51763809 |
| 2.6131259 | 0.76536686 |
| 2.7320508 | 1 |
| 2.8042295 | 1.2175229 |
| 2.8284271 | 1.4142136 |
| 2.8042295 | 1.5867067 |
| 2.7320508 | 1.7320508 |
| 2.6131259 | 1.8477591 |
| 2.4494897 | 1.9318517 |
| 2.2439421 | 1.9828897 |
| 2 | 2 |
| 1.7218373 | 1.9828897 |
| 1.4142136 | 1.9318517 |
| 1.0823922 | 1.8477591 |
| 0.73205081 | 1.7320508 |
| 0.36918382 | 1.5867067 |
| 2.220446e-16 | 1.4142136 |
| -0.36918382 | 1.2175229 |
| -0.73205081 | 1 |
| -1.0823922 | 0.76536686 |
| -1.4142136 | 0.51763809 |
| -1.7218373 | 0.26105238 |
| -2 | 2.4492936e-16 |
| -2.2439421 | -0.26105238 |
| -2.4494897 | -0.51763809 |
| -2.6131259 | -0.76536686 |
| -2.7320508 | -1 |
| -2.8042295 | -1.2175229 |
| -2.8284271 | -1.4142136 |
| -2.8042295 | -1.5867067 |
| -2.7320508 | -1.7320508 |
| -2.6131259 | -1.8477591 |
| -2.4494897 | -1.9318517 |
| -2.2439421 | -1.9828897 |
| -2 | -2 |
| -1.7218373 | -1.9828897 |
| -1.4142136 | -1.9318517 |
| -1.0823922 | -1.8477591 |
| -0.73205081 | -1.7320508 |
| -0.36918382 | -1.5867067 |
| -6.6613381e-16 | -1.4142136 |
| 0.36918382 | -1.2175229 |
| 0.73205081 | -1 |
| 1.0823922 | -0.76536686 |
| 1.4142136 | -0.51763809 |
| 1.7218373 | -0.26105238 |
| 2 | -4.8985872e-16 |
A marker can change shape substantially while preserving its area.
Simple shear combines shape change and rotation; principal stretches are not simply the diagonal entries of the deformation matrix. Stress, elastic recovery and brittle failure require material and loading information absent here.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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At γ=0 and radius 3, what are the principal stretches, semiaxes and area?
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