Construct a material representation without overclaiming evidence
Build individual substitution sites, preserve composition while changing arrangement, and identify what empirical properties cannot determine.
Learning outcome: Construct and critique an atom-count representation using a mass-to-atom reference and distinguish composition, arrangement and mobile charge.
Starting recap
Atom percent counts atoms; mass percent weighs them. A finite drawing has limited composition resolution and need not reveal a real crystal structure.
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Try
The source 10% nickel by mass row contains 10.73% nickel atoms. One nickel among eight sites is 12.5%, so an eight-site drawing cannot match it exactly.
Open the experimentPredict
Before editing, state how many nickel sites give the nearest eight-site composition. Predict whether moving that site changes the count, real material resistivity, or the information justified by the packet.
Experiment
Build and capture your own diagram. Make a second arrangement with the same count, then a two-nickel arrangement with different adjacent contacts. Explain the difference between a teaching contact count and a measured structure. Transfer to the 5% mass target and explain the coarse nearest-count result.
Build and challenge a particulate representation
Evaluated material reference values · original wire and site representations · Eight editable substitution sites form an original counting cartoon, not the crystal structure of copper–nickel. Site arrangements never generate empirical resistivity.
Reset keeps your prediction, captures and practice history.
Your editable substitution-site diagram
Target Cu–10% Ni, 293 K: 10% nickel by mass corresponds to the source's 10.73% nickel atoms. Select individual sites to replace Cu by Ni. Every site holds one atom; no interstitial site is introduced. Keyboard users can Tab to a site and press Space.
0/8 = 0% nickel sites. Difference from the atomic target: -10.73 percentage points. One site is 12.5 percentage points, so exact matching may be impossible. The nearest count is 1; a zero nearest count for a dilute alloy reflects this coarse representation, not absence of nickel in the material.
The boxes are counting positions, not a square crystal or measured atom sizes. Positive metal cores coexist with delocalized electrons; the labels name the elements, not formal oxidation states. The electron band is a qualitative carrier representation, not a measured electron count, drift rate or trajectory. In a solid ionic model the ions occupy constrained sites; mobile ions in a melt or solution provide another conduction mechanism. Conductivity alone does not uniquely identify bonding.
There are 0 unlike-element contacts among 10 horizontal/vertical edges in this cartoon. Capture a diagram, then move nickel sites while keeping their count fixed. Compare the count and contact ledger. This edge count is not a real coordination number, clustering measurement or resistivity predictor.
The selected empirical resistivity stays 13.89 × 10⁻⁸ Ω m regardless of your drawing. An arbitrary clustered diagram may not represent the source preparation. Explain what diffraction or preparation evidence you would request before claiming a unique structure. Save both diagrams with those explanations as captures.
| Material / T | Ni mass % / atom % | ρ / 10⁻⁸ Ω m | Source estimated uncertainty |
|---|---|---|---|
| Pure Cu, 293 K | 0 / 0 | 1.678 | ±0.5% |
| Cu–0.5% Ni, 293 K | 0.5 / 0.54 | 2.23 | ±5% |
| Cu–1% Ni, 293 K | 1 / 1.08 | 2.85 | ±5% |
| Cu–3% Ni, 293 K | 3 / 3.24 | 5.32 | ±5% |
| Cu–5% Ni, 293 K | 5 / 5.39 | 7.77 | ±5% |
| Cu–10% Ni, 293 K | 10 / 10.73 | 13.89 | ±5% |
| Pure Cu, 400 K | 0 / 0 | 2.398 | ±1% |
| Cu–10% Ni, 400 K | 10 / 10.73 | 14.81 | ±3% |
Source definitions and comparison limits
Ho et al. (1983), Electrical Resistivity of Ten Selected Binary Alloy Systems, Table 4, printed p. 228. Accessed 2026-10-28. Recommended, smoothed reference values for well-homogenized alloys with low clustering, without severe quenching or cold work. Pure copper is well-annealed and high-purity. Room-temperature dimensions are used without thermal-expansion correction (printed pp. 187–188, 227, 240). Exact impurity concentrations, pressure, common specimen preparation and covariance are not specified for these recommended rows. The stated percentages are source estimated uncertainties, not declared confidence intervals. All selected rows are unstarred; source stars elsewhere flag temperature ranges without experimental data. These values are evaluated recommendations, not a new raw-data cohort. Only selected factual numbers are reproduced; diagrams and tasks are original.
Your diagram has 0 nickel sites among eight.
Compare a second arrangement with the same count. Equal composition does not mean equal microscopic arrangement; the reference does not determine a unique diagram.
Captures retain your reference comparison and wire geometry or each editable substitution site. Replay recalculates the source comparison and your counting representation; it does not measure a new alloy, infer a unique structure or grade the explanation.
Understand
Apply
Public practice checks a specific claim. It does not establish independent mastery.
Combine a numerical source comparison, two independently constructed diagrams, and a competing explanation. Distinguish mobile metallic electrons from mobile ions in a liquid and propose additional evidence needed for an unfamiliar conducting material.
Continue
Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.
Skipping retains experiments and awards no mastery.
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