Determine molecular polarity from vector evidence
Combine declared bond vectors and test how asymmetric contributions break cancellation.
Learning outcome: Compare equal and unequal dipoles in linear, trigonal-planar and tetrahedral templates. Then compare equal trigonal-planar and trigonal-pyramidal arrangements, retaining all three components.
Starting recap
Review the electron and formal-charge budget, bond multiplicity, signed interaction energies and the distinction between a model and a measured property.
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Try
Two equal opposite unit bond dipoles sum to zero; changing the first magnitude to2 leaves a net magnitude1, although their magnitude sum is3.
Open the experimentPredict
Does a symmetric drawing guarantee cancellation when bond-dipole magnitudes differ?
Experiment
Compare equal and unequal dipoles in linear, trigonal-planar and tetrahedral templates. Then compare equal trigonal-planar and trigonal-pyramidal arrangements, retaining all three components.
Add bond-dipole vectors rather than magnitudes
Worked teaching model · synthetic values · Each bonded direction has outward dipole magnitude 1 except the first selected control. This explicitly stipulated vector model omits other electronic contributions. Chemical dipole-arrow conventions can differ; here all vectors use one declared outward convention. Molecular net is the vector sum, not sum of magnitudes.
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Orthographic projection: bonds toward the viewer use thicker lines; dashed outlined sites are lone-pair domains. Overlap in a view does not merge sites. The table retains depth coordinates. Ideal domain directions are not measured bond angles.
| Site | x | y | z |
|---|---|---|---|
| bond 1 | 0.8660254 | 0 | -0.5 |
| bond 2 | -0.8660254 | 0 | 0.5 |
| Contribution | x | y | z |
|---|---|---|---|
| bond 1 | 1 | 0 | 0 |
| bond 2 | -1 | 0 | 0 |
The geometry diagram shows unit bond directions, not dipole magnitudes. Use these weighted components and the net ledger to compare cancellation.
Axes rescale. Connected samples represent the supplied continuous parameter relationship; stems denote discrete pairs or steps, not a time trajectory.
Numerical plot coordinates
| unordered bonded pair index | ideal angle (degrees) |
|---|---|
| 1 | 180 |
| Quantity | Value | Unit |
|---|---|---|
| Total electron domains | 2 | domains |
| Bonded atoms | 2 | atoms |
| Lone-pair domains | 0 | domains |
| Smallest ideal bond angle | 180 | degrees |
| Largest ideal bond angle | 180 | degrees |
| Net dipole x | 0 | relative units |
| Net dipole y | 0 | relative units |
| Net dipole z | 0 | relative units |
| Net dipole magnitude | 0 | relative units |
| Sum of dipole magnitudes | 2 | relative units |
AX2 linear
Components use the unrotated model axes; the diagram camera changes their appearance, not the vector sum. Equal symmetric bond contributions can cancel; unequal magnitudes break that cancellation. Lone-pair electronic contributions are not separately computed, so this is a declared bond-vector model, not an ab initio molecular dipole.
AX2 linear
Components use the unrotated model axes; the diagram camera changes their appearance, not the vector sum. Equal symmetric bond contributions can cancel; unequal magnitudes break that cancellation. Lone-pair electronic contributions are not separately computed, so this is a declared bond-vector model, not an ab initio molecular dipole.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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Public practice checks a specific claim. It does not establish independent mastery.
What electronic contributions or structural changes are omitted by a simple bond-vector sum?
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