Infer mass from a force–acceleration relationship
Newton’s second law relates the net force on a fixed-mass object to its acceleration: Fnet=ma. The word net matters. A pulling-force reading alone is not net force when friction or another horizontal interaction also acts. Before fitting mass, specify which forces the sensor includes and which must be subtracted.
Learning outcome: Hold mass fixed while varying offset; compare slopes using two well-separated data points. Then hold offset fixed and change mass. Explain which graph feature changes in each intervention. Write a calibration test that could distinguish a sensor offset from an actual constant opposing force.
Starting recap
Review signed vectors, components, acceleration, graph slopes and system boundaries. Every force must name its agent and recipient.
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For assigned mass 3 kg and offset 2 N, readings at accelerations 0,1,2,3 m/s² are 2,5,8,11 N. Using the endpoints gives mass=(11−2)/(3−0)=3 kg. A one-point estimate at 1 m/s² would give 5 kg; at 3 m/s² it would give 11/3 kg. Their inconsistency reveals the missing intercept.
Open the experimentPredict
Will adding a constant 2 N sensor offset change the fitted slope or only the intercept?
Experiment
Hold mass fixed while varying offset; compare slopes using two well-separated data points. Then hold offset fixed and change mass. Explain which graph feature changes in each intervention. Write a calibration test that could distinguish a sensor offset from an actual constant opposing force.
Infer inertial mass despite a force-sensor offset
Worked teaching model · synthetic values · Synthetic exact data F_read=m a+offset at accelerations 0,1,2,3 m/s². The force sensor reads net horizontal force plus a constant offset. Acceleration calibration is exact; no random uncertainty or speed-dependent drag.
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Axes rescale with settings; use values, not screen angles. In the mass-position display, the dashed vertical line marks the center-of-mass coordinate, not an extra object.
| acceleration (m/s²) | sensor force reading (N) |
|---|---|
| 0 | 2 |
| 1 | 5 |
| 2 | 8 |
| 3 | 11 |
| Quantity | Value | Unit |
|---|---|---|
| Slope-inferred mass | 3 | kg |
| Intercept-inferred sensor offset | 2 | N |
| Naive F/a mass at a=1 m/s² | 5 | kg |
| Naive F/a mass at a=3 m/s² | 3.66667 | kg |
A constant sensor offset changes the intercept, not the slope; dividing one uncorrected reading by acceleration biases mass.
Use ΔF_read/Δa rather than F_read/a when the zero is uncertain. This ideal line cannot distinguish all real calibration errors; an acceleration scale error would change the slope.
A constant sensor offset changes the intercept, not the slope; dividing one uncorrected reading by acceleration biases mass.
Use ΔF_read/Δa rather than F_read/a when the zero is uncertain. This ideal line cannot distinguish all real calibration errors; an acceleration scale error would change the slope.
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Public practice checks a specific claim. It does not establish independent mastery.
Why would an acceleration-scale error bias the inferred mass even if the force-sensor intercept were corrected?
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