Infer density without confusing sample mass and tare
Solids, liquids and gases differ because of particle arrangements, motion and interactions. A solid resists sustained shape change; a liquid flows while retaining approximately fixed volume; a gas flows and can change volume substantially. Liquids and gases are fluids. An ideal fluid in this course is incompressible and has no viscosity, an approximation rather than a claim that real materials lack internal interactions.
Learning outcome: Compare tare 0 and0.10 kg at density1000, then density500 and1500 at fixed tare. Retain two sample points and the zero-volume point; derive the slope and intercept rather than reading one ratio. Explain why the dashed sample-only curve differs from the observed curve.
Starting recap
Review density and unit conversion, perpendicular force components, static force balance, work-energy, mass conservation and projectile motion.
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Try
Original observations at volumes 0.0002 and 0.0006 m³ are 0.30 and 0.70 kg. The slope is (0.70−0.30)/(0.0006−0.0002)=1000 kg/m³; intercept is 0.10 kg. Using the first raw ratio gives 1500 kg/m³, which mistakes the offset for sample mass.
Open the experimentPredict
Can an unchanged tare error alter a graph intercept without altering its slope?
Experiment
Compare tare 0 and0.10 kg at density1000, then density500 and1500 at fixed tare. Retain two sample points and the zero-volume point; derive the slope and intercept rather than reading one ratio. Explain why the dashed sample-only curve differs from the observed curve.
Separate density slope from a mass offset
Worked teaching model · synthetic values · Original sample volumes 0–0.001 m³ with observed mass=ρV+tare. Exact synthetic volumes and constant additive mass offset. The offset is not sample mass; no mixing-volume contraction or density variation is modeled.
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Axes rescale with settings; compare numerical values, not screen angles or apparent lengths. Solid/points show the selected model relationship or observations; the dashed comparison is explained below.
| Quantity | Value | Unit |
|---|---|---|
| Density from mass-volume slope | 1000 | kg/m³ |
| Mass-axis intercept | 0.1 | kg |
| Observed mass at volume0.001 m³ | 1.1 | kg |
| Naive mass/volume at0.001 m³ | 1100 | kg/m³ |
Accessible plot coordinates
| sample volume (m³) | observed mass (kg) |
|---|---|
| 0 | 0.1 |
| 0.0002 | 0.3 |
| 0.0004 | 0.5 |
| 0.0006 | 0.7 |
| 0.0008 | 0.9 |
| 0.001 | 1.1 |
| sample volume (m³) | observed mass (kg) |
|---|---|
| 0 | 0 |
| 0.0002 | 0.2 |
| 0.0004 | 0.4 |
| 0.0006 | 0.6 |
| 0.0008 | 0.8 |
| 0.001 | 1 |
Density is the slope; an unremoved constant tare changes the intercept and corrupts a single mass/volume ratio.
Solid, liquid and gas behavior reflects particle interactions. Liquids and gases flow, but the ideal fluid here is incompressible and inviscid; real gases are often compressible. Average density m/V is not necessarily the local density of a heterogeneous object.
Density is the slope; an unremoved constant tare changes the intercept and corrupts a single mass/volume ratio.
Solid, liquid and gas behavior reflects particle interactions. Liquids and gases flow, but the ideal fluid here is incompressible and inviscid; real gases are often compressible. Average density m/V is not necessarily the local density of a heterogeneous object.
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Understand
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Public practice checks a specific claim. It does not establish independent mastery.
Which observations could distinguish a constant tare error from density that actually changes with sample volume?
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