Physics for ME · Chapter 15 of 16 · Advanced · Experimental thinking
Measurement, Uncertainty, and Experimental Physics
An experiment is an argument with evidence. This chapter teaches the rules of evidence: instruments, errors, and the honest propagation of doubt.
Readiness check
From Chapter 1 and Math Chapters 6 and 15. Tick only what you can do closed-notes.
- Hold the significant-figures discipline.
- Compute mean and standard deviation of a small sample (Math Chapter 15).
- Use the total differential for sensitivities (Math Chapter 6).
- Distinguish random scatter from a fixed offset.
- Convert relative and absolute uncertainties.
The core idea
Every measurement is value plus doubt. Derived quantities inherit doubt through their formulas.
urel(xⁿ) = n·urel(x)uf = √(Σ(∂f/∂x·ux)²)For products and powers, relative uncertainties combine in quadrature, with exponents as multipliers (the d² in an area doubles d's contribution). Random error shrinks with repeats; systematic error (bias) only yields to calibration.
What this chapter covers
- 15.1 Instruments and resolution: what the last digit really promises.
- 15.2 Random versus systematic error: the two diseases.
- 15.3 Repeats and statistics: Math Chapter 15 at the bench.
- 15.4 Propagation of uncertainty: doubt through formulas, exponents included.
- 15.5 Reporting results: value ± uncertainty, with units and confidence.
- 15.6 Designing better measurements: attacking the dominant term.
Engineering connection: instrumentation, lab courses, quality control; bridge reference Taylor, An Introduction to Error Analysis.
Worked example: what metal is this cylinder?
A cylinder is measured: m = 155.0 ± 0.5 g, diameter d = 25.04 ± 0.05 mm, length L = 40.1 ± 0.1 mm. Find its density with uncertainty and identify the material.
- ProblemFind ρ and uρ for the cylinder in Figure 1 and name the material.
- Given / findm, d, L with uncertainties above. Find ρ ± u.
- AssumptionsIndependent uncertainties; a true cylinder; instruments calibrated (bias addressed separately).
- Modelρ = 4m/(πd²L). Relative uncertainties add in quadrature with d's doubled by its exponent.
- Equationsurel(ρ) = √(um² + (2ud)² + uL²)
- SolveV = π × 25.04² × 40.1/4 = 19 748 mm³ = 19.75 cm³. ρ = 155.0/19.75 = 7.849 g/cm³. Relative doubts: m 0.32%, d 0.20% (doubled: 0.40%), L 0.25%. Combined: √(0.32² + 0.40² + 0.25²) = 0.57%, so u = 0.045. ρ = 7.85 ± 0.05 g/cm³.
- CheckSteel sits at 7.85; aluminium (2.70), brass (8.5), and copper (8.96) all fall far outside the band. The dominant doubt is the diameter, exactly because it enters squared.
- ConclusionThe material verdict is defensible because the uncertainty band excludes the alternatives. To tighten the result, attack d first (a micrometer instead of calipers): designing the next measurement from the budget is the whole craft.
Misconceptions and diagnostics
| Mistake | Symptom | Diagnostic question | Correction |
|---|---|---|---|
| Resolution mistaken for accuracy | Five digits trusted from an uncalibrated meter | "Fine display, but is the reading true?" | Resolution is the step size; accuracy needs calibration against a standard. |
| Exponents ignored in propagation | d's doubt counted once under a square | "What power does this input carry?" | Relative uncertainty multiplies by the exponent: the d² doubled it here. |
| Uncertainties added linearly | Doubt budgets pessimistically fat | "Are these error sources independent?" | Independent doubts combine in quadrature (the root-sum-square), not by addition. |
| One reading treated as truth | No repeats, no scatter estimate | "What would a second measurement show?" | Repeat at least a few times; scatter is data about your own measurement. |
Practice ladder
A voltage is 12.06 ± 0.05 V and a current 2.31 ± 0.02 A. Find the power and its uncertainty.
Show answer
P = 27.86 W. Relative: √(0.41%² + 0.87%²) = 0.96%, so u = 0.27. P = 27.9 ± 0.3 W.
The pendulum formula g = 4π²L/T² is used with L = 1.000 ± 0.002 m and T = 2.007 ± 0.005 s. Which input dominates the doubt in g, and what is g ± u?
Show answer
g = 4π² × 1.000/4.028 = 9.80 m/s². Relative: L gives 0.2%; T, squared, gives 2 × 0.25% = 0.5%: T dominates. Combined 0.54%: g = 9.80 ± 0.05 m/s². Time the swing better before measuring the string better.
The Chapter 11 kettle experiment gave c = 4500 J/kg·K versus the true 4186. Scatter across repeats was only ±100. Diagnose: random or systematic, and name the likely bias.
Show answer
The 314 J/kg·K excess is three times the scatter: systematic. Likely bias: heat lost to the kettle body and air is charged to the water, inflating c. Averaging more runs would never fix it; insulating or accounting for the kettle would.
Design and run an indirect measurement of your own (density of a coin, g from a phone-timed drop, spring constant from masses and a ruler). Produce the full uncertainty budget and state the dominant term and your next improvement.
What good work looks like
The formula with all inputs and doubts, exponents handled, quadrature shown, the result with the band, and a concrete next-instrument recommendation aimed at the dominant term.
Working with AI, and proving it yourself
Use AI as an examiner, not a solver
Portfolio task
Write the cylinder-density experiment (or your Level 4 design) as a one-page lab report in the professional format: aim, apparatus with resolutions, data, propagation, result with band, comparison, and the next-improvement recommendation.
Retrieval and spaced review
Closed notes. Answer out loud, then reveal.
1. Resolution, precision, accuracy: define and separate.
Resolution: smallest displayed step. Precision: repeatability (scatter). Accuracy: closeness to truth (bias). All three are independent properties.
2. Which error type does averaging cure, and which does it not?
Averaging shrinks random error by √n; it never touches systematic bias.
3. How do relative uncertainties combine for products and powers?
In quadrature, each multiplied by its exponent: urel = √(Σ(nᵢ·urel,i)²).
4. What is the correct way to report a measured result?
Value ± uncertainty with units and the confidence basis, rounded so the uncertainty has one or two significant figures.
5. Given a finished budget, how do you improve the experiment?
Attack the dominant term: better instrument or method for that one input. Improving the others buys almost nothing.
Textbook mapping
| Item | Mapping |
|---|---|
| Main source | OpenStax University Physics Vol. 1, Units and Measurement (uncertainty sections) |
| Bridge reference | Taylor, An Introduction to Error Analysis: the serious treatment, strongly recommended |
| Core topics | 15.1 Instruments and resolution · 15.2 Error types · 15.3 Repeats · 15.4 Propagation · 15.5 Reporting · 15.6 Designing better measurements |
| Engineering connection | Instrumentation and lab courses, quality control, reliability; twin of Math Chapter 15. |
| Read next | Chapter 16: Optics, Light, and Modern Physics Overview (short, optional). |