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designing a reproducible physical investigation

Learning objectives

  • Outcome

    Formulate a research question and a testable hypothesis, and identify the independent, dependent and controlled variables.

  • Outcome

    Write an operational measurement protocol specifying the instrument, its resolution, the number of trials NN, and how uncertainty is estimated.

  • Outcome

    Evaluate whether someone else's procedure is reproducible by deciding whether another investigator could repeat it from the written description alone.

  • Outcome

    Distinguish systematic from random error and propose actions, such as calibration and repeated trials, to reduce them.

Understand the idea

Designing a Reproducible Physical Investigation

Text

A reproducible investigation is one in which an independent researcher, given only the written protocol, obtains the same result within the stated uncertainty. Design begins with a research question tied to physical theory: theory indicates which quantities matter and which may be neglected. Variables must be classified as independent, dependent and controlled, and every quantity needs an operational definition, that is, the measurement procedure that fixes its value. The measurement protocol states the instrument, its resolution, calibration, the number of trials NN, and how the mean xˉ\bar{x} and uncertainty uu are computed. Reproducibility requires recording raw data, environmental conditions and the analysis model so that others can repeat or refute the work. Finally, systematic error shifts all readings in one direction and is addressed by calibration and comparison of methods, while random error is reduced by averaging over trials, with uncertainty decreasing roughly as u∝1/Nu \propto 1/\sqrt{N}.

Worked examples

Direct

Problem

Five independent length readings are given: 12.4, 12.5, 12.3, 12.5, 12.3 cm. Compute the mean value and the standard uncertainty of the mean.

Solution

Mean value: xˉ=12.4+12.5+12.3+12.5+12.35=12.40 cm.\bar{x} = \frac{12.4+12.5+12.3+12.5+12.3}{5} = 12.40\ \text{cm}. Deviations from the mean: 0, +0.1, −0.1, +0.1, −0.10,\ +0.1,\ -0.1,\ +0.1,\ -0.1 cm. Sample standard deviation: s=02+0.12+0.12+0.12+0.125−1=0.10 cm.s = \sqrt{\frac{0^2+0.1^2+0.1^2+0.1^2+0.1^2}{5-1}} = 0.10\ \text{cm}. Standard uncertainty of the mean: u=sN=0.105≈0.045 cm.u = \frac{s}{\sqrt{N}} = \frac{0.10}{\sqrt{5}} \approx 0.045\ \text{cm}. Reported measurement: L=(12.40±0.05)L = (12.40 \pm 0.05) cm. This protocol is reproducible because all readings, the averaging formula and the uncertainty rule are stated.

Application

Problem

Design a reproducible investigation of whether the period of a simple pendulum depends on amplitude at fixed length and mass. Identify the variables, the measurement protocol and the uncertainty estimate.

Solution

Variables. Independent: initial amplitude θ0\theta_0; dependent: period TT; controlled: string length L=0.500L = 0.500 m, bob mass m=50m = 50 g, release without a push, the same timing instrument.

Protocol. Deflect the pendulum to θ0\theta_0 and release it from rest. Measure the time tt for Nosc=10N_{\text{osc}} = 10 full oscillations, so T=t/NoscT = t/N_{\text{osc}}. Repeat N=5N = 5 times at each amplitude, for example θ0=5∘\theta_0 = 5^\circ and θ0=20∘\theta_0 = 20^\circ. Record the resolution of the stopwatch or photogate and the temperature.

Analysis. For each amplitude compute Tˉ\bar{T} and u=s/Nu = s/\sqrt{N}. Theory gives T0=2πL/g≈1.42T_0 = 2\pi\sqrt{L/g} \approx 1.42 s and the correction T≈T0(1+θ02/16)T \approx T_0\left(1+\theta_0^2/16\right): at 5∘5^\circ the effect is about 0.05%, at 20∘20^\circ about 0.8% (the period is less than 1% longer than the small-angle value). Therefore many oscillations must be timed in order to resolve such small changes. Claim a dependence only when the difference of the means exceeds the combined uncertainty.

Transfer

Problem

A report says: We measured the resistance with a multimeter and got about 10 ohms; the result matched theory. Rewrite this as a reproducible protocol and state what data and uncertainty estimates must be added.

Solution

What is missing. The sample, instrument, range, resolution, connection scheme, temperature, number of readings and the method of comparison with theory are not stated. Without them the experiment cannot be repeated.

Rewritten protocol. Sample: a wire of length L=(1.000±0.001)L = (1.000 \pm 0.001) m and diameter d=(0.500±0.005)d = (0.500 \pm 0.005) mm; the material is specified, temperature $T = (20 \pm 1)^\circ$C. Instrument: digital multimeter, resistance mode, 200 ohm range, resolution 0.1 ohm, calibrated against a reference resistor. Perform measurements in a four-wire configuration to exclude lead resistance; take N=10N = 10 readings and record every value.

Analysis and uncertainty. Compute Rˉ\bar{R} and uR=s/Nu_R = s/\sqrt{N}, together with the instrument contribution. Obtain the theoretical value from the model R=ρL/AR = \rho L/A, where A=πd2/4A = \pi d^2/4; estimate the theoretical uncertainty through LL, dd and the tabulated value of ρ\rho. A comparison is valid only if the raw data, conditions and all uncertainty contributions are recorded; then another investigator can repeat the measurement and check the conclusion.

Practice

Text

Safe self-study plan. Work with a simulation, for example a pendulum or circuit model, so that you never deal with mains voltage, lasers or high temperatures. Choose one research question, state a hypothesis and list the independent, dependent and controlled variables. Write a protocol: the instrument or simulation settings, resolution, number of trials NN, and the averaging rule. Run N≥5N \ge 5 trials at each point, record the raw data in a table, and compute xˉ\bar{x} and u=s/Nu = s/\sqrt{N}. Then test reproducibility: give the protocol to a peer or repeat the experiment a few days later without changing the protocol text, and compare the results within the stated uncertainty.

Visual reference

Purpose

Show the structure of a reproducible investigation and the place of each element, from question and variables to the reproducibility check.

Representation

Block diagram, left to right: Question →\to Hypothesis and theory →\to Variables (independent xx, dependent yy, controlled cic_i) →\to Protocol (instrument, resolution, NN, calibration) →\to Raw data →\to Analysis (xˉ\bar{x}, uu) →\to Reproducibility check. Below it, a data table with columns ii, xix_i, yiy_i, notes, and underneath the formula u=s/Nu = s/\sqrt{N}.

Real-world examples

Timing a $100\,\text{m}$ sprint with repeated trials

Scenario

A student times a classmate over 100 m100\,\text{m} on the same school track. Three runs give t1=12.4 st_1 = 12.4\,\text{s}, t2=12.6 st_2 = 12.6\,\text{s}, t3=12.3 st_3 = 12.3\,\text{s}, with mean tˉ=12.43 s\bar t = 12.43\,\text{s}. The stopwatch is started when the rear hand leaves the ground and stopped when the chest crosses the finish line; the timer's reaction adds roughly 0.2 s0.2\,\text{s} to every reading. To make the result reproducible, the same starter, the same painted line, and the same stopwatch are used, and every run starts from a standing position after the same countdown.

Connection

The scenario exercises operational definitions: 'start' and 'finish' must be fixed by a rule, not by intuition. Repeated trials estimate random scatter around tˉ\bar t, while the reaction time is a systematic offset that shifts all three values in the same direction. A reproducible investigation states both the protocol and the uncertainty.

Cooling curve of water in a mug

Scenario

250 mL250\,\text{mL} of water at 90 ∘C90\,^\circ\text{C} are poured into a ceramic mug in a room at 22 ∘C22\,^\circ\text{C}. Every 60 s60\,\text{s} a digital thermometer with resolution 0.5 ∘C0.5\,^\circ\text{C} is read at the same depth: 9090, 8282, 7575, 6969, 64 ∘C64\,^\circ\text{C}. Reproducibility requires the same mug, the same volume, the same starting temperature, and a note whether the lid is on or off.

Connection

Control of variables is the core of the design: volume, container, and room temperature are held constant, so time is the only independent variable and temperature the dependent one. The thermometer's 0.5 ∘C0.5\,^\circ\text{C} resolution sets the measurement uncertainty, and the written protocol lets another student repeat the same curve.

Braking distance on a bicycle

Scenario

A cyclist rides at 5.0 m/s5.0\,\text{m/s} on dry asphalt and brakes fully; chalk marks give braking distances 3.2 m3.2\,\text{m}, 3.4 m3.4\,\text{m}, 3.1 m3.1\,\text{m}. Each run uses the same bike, tire pressure 3.0 bar3.0\,\text{bar}, rider mass 60 kg60\,\text{kg}, and the same braking technique from the moment the lever is pulled to the stop. Air temperature is 25 ∘C25\,^\circ\text{C} and wind 1 m/s1\,\text{m/s}.

Connection

The design isolates speed as the independent variable by fixing mass, tires, and surface; three repeats expose random variation about 3.23 m3.23\,\text{m}. This is where theory guides the choice of variables: kinetic energy and friction predict that speed matters, so other factors are controlled rather than varied.