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SCIENCE · INVESTIGATE AND EXPLAIN

Fit two hypotheses before revealing a third location

Two calibrated models can fit the same two records perfectly and still make different predictions elsewhere. At exact perpendicular distances y=1,2,3 m, compare a known-half-length 1 m straight-segment shape f(y)=1/[y√(L²+y²)] with L=1 m with an infinite-line shape g(y)=1/y. Each has its own unknown amplitude and constant indicated baseline. The finite-shape amplitude has units µT m², while the infinite-line amplitude has units µT m; these coefficients are not interchangeable.

Learning outcome: Fit both amplitudes and baselines from only distances 1 and 2. Freeze both third-distance predictions and propagate ±0.005 µT calibration bounds. Then compare the unused third observation, retaining any additional observation uncertainty. State an independent measurement needed to separate background from instrument offset.

Starting recap

Review cross products, source integration measures, line integrals, differential initial states and signed work. Distinguish symmetry premises from integral laws.

All lessons are open directly. Your saved experiments remain when you leave and return.

Try

Take generating current 3 A and baseline 0.1 µT. The first two indicated fields are 0.1+0.6/√2 and 0.1+0.6/(2√5) µT. Both candidates fit these exactly. The finite-segment third prediction is 0.1+0.6/(3√10)≈0.163246 µT; the infinite-line fit gives a different third value because its shape decays differently after the baseline is fitted.

Open the experiment

Predict

Why can the third reading compare these two calibrated hypotheses?

Experiment

Fit both amplitudes and baselines from only distances 1 and 2. Freeze both third-distance predictions and propagate ±0.005 µT calibration bounds. Then compare the unused third observation, retaining any additional observation uncertainty. State an independent measurement needed to separate background from instrument offset.

Fit two spatial hypotheses and reserve a third location

Worked teaching model · synthetic values · Perpendicular readings at exact distances 1,2,3 m. Generator is the known-half-length 1 m segment contribution plus constant baseline; real return/background fields are not uniquely identified. Both candidate models fit amplitude and baseline using only distances 1,2. Distance 3 is withheld. Field gain is stipulated calibrated; baseline may represent sensor offset or an approximately uniform background.

Reset keeps your prediction, captures and practice history.

Two calibrated hypotheses and one unused location

indicated field (microtesla)perpendicular distance (m)030.52426410

Unlike graph quantities rescale independently; read units and values, not screen angles. 1: finite known-length fit (solid).2: infinite-line fit (dashed).3: fresh third-distance observation (open-circle marked location). Joined curves show the supplied model, not additional observations.

Equivalent numerical coordinates for Two calibrated hypotheses and one unused location

finite known-length fit

perpendicular distance (m)indicated field (microtesla)
10.5242641
1.0250.5087749
1.050.4940887
1.0750.480151
1.10.4669124
1.1250.4543274
1.150.4423541
1.1750.4309542
1.20.4200922
1.2250.4097354
1.250.3998536
1.2750.3904188
1.30.381405
1.3250.372788
1.350.3645456
1.3750.3566567
1.40.3491021
1.4250.3418635
1.450.334924
1.4750.3282678
1.50.3218801
1.5250.315747
1.550.3098556
1.5750.3041936
1.60.2987496
1.6250.2935129
1.650.2884734
1.6750.2836215
1.70.2789483
1.7250.2744454
1.750.2701048
1.7750.265919
1.80.261881
1.8250.257984
1.850.2542217
1.8750.2505882
1.90.2470778
1.9250.2436851
1.950.2404051
1.9750.237233
20.2341641
2.0250.2311942
2.050.2283191
2.0750.225535
2.10.2228382
2.1250.220225
2.150.2176923
2.1750.2152367
2.20.2128553
2.2250.2105452
2.250.2083036
2.2750.2061279
2.30.2040155
2.3250.2019642
2.350.1999715
2.3750.1980355
2.40.1961538
2.4250.1943247
2.450.1925462
2.4750.1908165
2.50.1891338
2.5250.1874965
2.550.1859029
2.5750.1843517
2.60.1828413
2.6250.1813704
2.650.1799375
2.6750.1785414
2.70.177181
2.7250.1758549
2.750.1745621
2.7750.1733015
2.80.1720721
2.8250.1708728
2.850.1697027
2.8750.1685608
2.90.1674463
2.9250.1663584
2.950.1652961
2.9750.1642588
30.1632456

At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.

infinite-line fit

perpendicular distance (m)indicated field (microtesla)
10.5242641
1.0250.5101128
1.050.4966355
1.0750.483785
1.10.4715186
1.1250.4597974
1.150.4485858
1.1750.4378513
1.20.4275641
1.2250.4176967
1.250.4082241
1.2750.3991229
1.30.3903718
1.3250.3819509
1.350.3738419
1.3750.3660277
1.40.3584926
1.4250.351222
1.450.344202
1.4750.33742
1.50.3308641
1.5250.3245231
1.550.3183867
1.5750.312445
1.60.3066891
1.6250.3011102
1.650.2957004
1.6750.2904521
1.70.2853582
1.7250.2804119
1.750.2756069
1.7750.2709373
1.80.2663974
1.8250.2619819
1.850.2576857
1.8750.2535041
1.90.2494325
1.9250.2454667
1.950.2416025
1.9750.2378362
20.2341641
2.0250.2305826
2.050.2270885
2.0750.2236785
2.10.2203498
2.1250.2170994
2.150.2139245
2.1750.2108227
2.20.2077914
2.2250.2048281
2.250.2019307
2.2750.199097
2.30.1963249
2.3250.1936125
2.350.1909577
2.3750.1883588
2.40.1858141
2.4250.1833218
2.450.1808804
2.4750.1784883
2.50.1761441
2.5250.1738463
2.550.1715935
2.5750.1693845
2.60.1672179
2.6250.1650927
2.650.1630075
2.6750.1609613
2.70.158953
2.7250.1569815
2.750.1550459
2.7750.1531452
2.80.1512784
2.8250.1494446
2.850.147643
2.8750.1458728
2.90.144133
2.9250.1424231
2.950.140742
2.9750.1390893
30.1374641

At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.

fresh third-distance observation

perpendicular distance (m)indicated field (microtesla)
30.1632456

At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.

Calculated quantities under the declared measurement model
QuantityValueUnit
First calibration field0.5242641microtesla
Second calibration field0.2341641microtesla
Fitted finite-segment current3A
Fitted finite-segment baseline0.1microtesla
Fitted infinite-line amplitude0.5802microtesla m
Fitted infinite-line baseline-0.05593591microtesla
Fresh third observation0.1632456microtesla
Finite-segment third prediction0.1632456microtesla
Infinite-line third prediction0.1374641microtesla
Infinite-line fresh residual0.02578147microtesla
Finite prediction calibration-error bound0.007444624microtesla
Infinite prediction calibration-error bound0.008333333microtesla

Both two-parameter hypotheses fit the first two records exactly; only the unused spatial record compares their predictions.

Each candidate has shape f(y), amplitude A and constant baseline B0. Solve A=(Y1−Y2)/(f1−f2), B0=Y1−A f1, then freeze Y3pred=wY1+(1−w)Y2 where w=(f3−f2)/(f1−f2). Independent ±0.005 microtesla calibration bounds propagate as epsilon(|w|+|1−w|); a fresh observation error would be additional. Segment half-length is stipulated independently, not inferred from these same two readings. A constant fitted baseline does not distinguish sensor offset from uniform background or prove omitted return fields are constant.

Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.

Both two-parameter hypotheses fit the first two records exactly; only the unused spatial record compares their predictions.

Each candidate has shape f(y), amplitude A and constant baseline B0. Solve A=(Y1−Y2)/(f1−f2), B0=Y1−A f1, then freeze Y3pred=wY1+(1−w)Y2 where w=(f3−f2)/(f1−f2). Independent ±0.005 microtesla calibration bounds propagate as epsilon(|w|+|1−w|); a fresh observation error would be additional. Segment half-length is stipulated independently, not inferred from these same two readings. A constant fitted baseline does not distinguish sensor offset from uniform background or prove omitted return fields are constant.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Specify sources, directions and independent premises

Two calibrated models can fit the same two records perfectly and still make different predictions elsewhere. At exact perpendicular distances y=1,2,3 m, compare a known-half-length 1 m straight-segment shape f(y)=1/[y√(L²+y²)] with L=1 m with an infinite-line shape g(y)=1/y. Each has its own unknown amplitude and constant indicated baseline. The finite-shape amplitude has units µT m², while the infinite-line amplitude has units µT m; these coefficients are not interchangeable.

Derive the integral or vector evolution

For either shape h, fit amplitude A=(Y1−Y2)/(h1−h2) and baseline B0=Y1−Ah1 using only the first two fields. Then freeze the third prediction Ah3+B0 before revealing Y3. The finite segment half-length is stipulated independently; fitting that length too would add an unknown and consume additional calibration information.

Check energy, symmetry and evidence limits

The third prediction can be written wY1+(1−w)Y2, where w=(h3−h2)/(h1−h2). Independent calibration-reading bounds ε therefore contribute ε(|w|+|1−w|), and a fresh observation error must be added separately when comparing a residual. A constant fitted baseline cannot distinguish a sensor zero from uniform background, nor prove an omitted return-path field is actually constant.

Worked original case

Take generating current 3 A and baseline 0.1 µT. The first two indicated fields are 0.1+0.6/√2 and 0.1+0.6/(2√5) µT. Both candidates fit these exactly. The finite-segment third prediction is 0.1+0.6/(3√10)≈0.163246 µT; the infinite-line fit gives a different third value because its shape decays differently after the baseline is fitted.

Investigation

Fit both amplitudes and baselines from only distances 1 and 2. Freeze both third-distance predictions and propagate ±0.005 µT calibration bounds. Then compare the unused third observation, retaining any additional observation uncertainty. State an independent measurement needed to separate background from instrument offset.

Changed-case practice

Try the changed case before feedback

For the infinite-line candidate with exact fields Y1=0.5 µT at 1 m and Y2=0.3 µT at 2 m, predict the indicated field at 3 m in µT.

This practice is public and unsaved. A matching number does not verify understanding. Retain your explanation, assumptions and changed-case evidence in the separate course workspace.

Sources and boundaries

Original derivations and synthetic numerical evidence checked 31 October 2026 against the primary explanation. The rounded teaching permeability is not asserted to be an exact modern SI constant; NIST CODATA 2022 lists its measured uncertainty. No live electrical construction, beam, strong-magnet handling, medical or physical certification claim is requested. Public feedback remains separate from retained first work, critique, revision and fresh assigned evidence.

Apply

Why can the third reading compare these two calibrated hypotheses?

Public practice checks a specific claim. It does not establish independent mastery.

Which source geometry, symmetry, initial state or calibration premise is necessary, and what independent observation could reject it?

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

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