Resolve plate motion in a common reference frame
A plate boundary is a relationship between moving bodies, not a speed attached to one plate. In a local east–north frame, subtract velocity of plate A from plate B. Then project that relative vector onto a boundary normal directed from A toward B and a perpendicular tangent. Positive normal motion increases separation; negative normal motion closes it.
Learning outcome: Rotate the normal while holding the two plate velocities fixed. Reconstruct both projections, mark positive directions and compare their squared sum with relative speed squared. Explain what observations distinguish rifting, subduction and transform accommodation.
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Keep reference frames, material properties, path geometry and actual catalog evidence distinct. Infer only what the retained observations and stated model support.
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At a=40 and θ=30°, relative motion is (30,20) mm/yr. Opening is 35.9808 mm/yr, tangent 2.3205 mm/yr and speed √1300=36.0555 mm/yr. Components depend on boundary orientation, while speed does not.
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Can a boundary have a large relative speed but little opening?
Experiment
Rotate the normal while holding the two plate velocities fixed. Reconstruct both projections, mark positive directions and compare their squared sum with relative speed squared. Explain what observations distinguish rifting, subduction and transform accommodation.
Resolve relative plate motion across an oriented boundary
Worked teaching model · synthetic values · Invented local Cartesian velocities: plate A=(10,0), plate B=(a,20) mm/yr in one common frame. Unit normal points from A toward B at angle b; positive relative normal velocity opens the boundary. Tangent is 90 degrees counterclockwise from normal. No spherical Euler-pole reconstruction.
Reset keeps your prediction, captures and practice history.
Boundary kinematics require a relative velocity and an explicitly oriented normal.
Positive opening, negative convergence and tangential slip can coexist in oblique motion. Changing a common reference-frame velocity cancels in B minus A; changing boundary orientation does not. Kinematics alone does not identify the driving force.
| Quantity | Value | Unit |
|---|---|---|
| Relative east velocity | 30 | mm/yr |
| Relative north velocity | 20 | mm/yr |
| Opening normal component | 35.980762 | mm/yr |
| Counterclockwise tangent component | 2.3205081 | mm/yr |
| Relative speed | 36.055513 | mm/yr |
| x | y |
|---|---|
| 0 | 0 |
| 30 | 20 |
Boundary kinematics require a relative velocity and an explicitly oriented normal.
Positive opening, negative convergence and tangential slip can coexist in oblique motion. Changing a common reference-frame velocity cancels in B minus A; changing boundary orientation does not. Kinematics alone does not identify the driving force.
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Set B east velocity −20 and the normal due east. What are the normal and tangential components? Does adding (100,−50) mm/yr to both plate velocities change them?
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