Annus Mirabilis · Interactive critical edition in preparation
Random steps to diffusion
Add many independent steps and see a spread appear.
The independent-step argument
From random steps to diffusion
A coin gives only two possible next steps; a uniform law fills an interval; a Gaussian law has tails. Keep their step variance equal, and ask what survives after many independent steps.
Predict before the numbers
After many steps, what will changing the step law while keeping its variance do?
The result appears when you choose, say you have one in mind, or skip.
Observation buttons use the accepted setup, not unsubmitted draft edits. They return to the same trial, not a fresh sample.
Keeping a seed across step-law changes is a reproducible comparison, not a claim of independent trials. Shared links load settings only; they never start a calculation.
| Quantity | Accepted value |
|---|---|
| Step variance (μm²) | 0.25 |
| Step fourth moment (μm⁴) | 0.0625 |
| Diffusion coefficient (μm²/s) | 1.25 |
| Sample signed mean (μm) | 0.0005 |
| Sample mean square (μm²) | 0.9865 |
| Model mean square (μm²) | 1 |
| Model RMS displacement (μm) | 1 |
Static worked example
CurrentThese numbers match the current settings.
Model note
- Primary outputs stepMean, stepSecondMoment, stepFourthMoment, biasedMean: Host calculation (diffusion.kernelMoments). Owner diffusion.kernelMoments.
- Primary outputs diffusionCoefficient, biasedDiffusion, biasedDrift, biasedCenteredDiffusion, cauchyDiffusion: Host calculation (diffusion.kernelDiffusivity). Owner diffusion.kernelDiffusivity.
- Primary outputs stepKurtosis, walkerCount, sumKurtosis, agreementBound, withinBound, histogramEdges, histogramExact, traceTimes, comparisonSteps, comparisonSampleMsd, comparisonModelMsd, comparisonDistance, comparisonShape, continuumIntervals, fixedRatioSteps, requestDraws, reusedRecording, retainedBytes: Host calculation (bm05.measure). Owner bm05.measure.
- Primary outputs sampleMean, sampleMeanSquare, sampleRms: Host calculation (diffusion.ensembleMoments). Owner diffusion.ensembleMoments.
- Primary outputs modelMeanSquare, modelRms, elapsedTime: Host calculation (diffusion.randomWalkMoments). Owner diffusion.randomWalkMoments.
- Primary output samplingTerm: Host calculation (diffusion.dkwBound). Owner diffusion.dkwBound.
- Primary outputs walkPositions, traceDisplacements, recordingDraws: Host calculation (diffusion.recordWalks). Owner diffusion.recordWalks.
- Primary output kolmogorovDistance: Host calculation (diffusion.kolmogorovDistanceToGaussian). Owner diffusion.kolmogorovDistanceToGaussian.
- Primary output shapeTerm: Host calculation (diffusion.kolmogorovShapeTerm). Owner diffusion.kolmogorovShapeTerm.
- Primary outputs histogramCounts, histogramFrequencies, underflow, overflow: Host calculation (diffusion.displacementHistogram). Owner diffusion.displacementHistogram.
- Primary output histogramGaussian: Host calculation (diffusion.intervalProbability). Owner diffusion.intervalProbability.
- Primary outputs coinPositions, coinProbabilities, coinNumerators, coinDenominator: Host calculation (diffusion.coinWalkDistribution). Owner diffusion.coinWalkDistribution.
- Primary outputs continuumLimit, fixedStepCoefficients, fixedRatioCoefficients: Host calculation (diffusion.continuumLimit). Owner diffusion.continuumLimit.
- Primary output replayedDraws: Host calculation (diffusion.observeWalks). Owner diffusion.observeWalks.
- Seed 1905.
- Accepted input revision 1.
- Snapshot version 1.
- Not modeled: A continuous Langevin path; only independent steps of a chosen law.
- Show the code
Accepted Equal left/right jumps: 2000 walkers after 4 steps, model mean square 1 square micrometres.
Accepted trial: Equal left/right jumps; seed 1905; 2000 walkers; step RMS 0.5 μm; interval 0.1 s. Observed after 4 of 400 recorded steps. Elapsed time: 0.4 s.
Two reasons the histogram is not a perfect bell
For coin and uniform steps, a finite number of steps leaves a shape gap, even with infinitely many walkers. Gaussian steps are the exception: their sums are Gaussian already. A finite number of walkers adds sampling variation. Neither is hidden by renormalizing the histogram.
| Sample-to-Gaussian gap | 0.192 |
|---|---|
| Finite-step shape gap | 0.1875 |
| Sampling allowance | 0.043592 |
| Shape plus sampling allowance | 0.23109 |
This sample is within the declared shape-plus-sampling allowance. The sampling allowance has 99.9% coverage for one prespecified comparison under the model, not simultaneous coverage over every trial or observation.
Exact coin probabilities after 4 steps
| Displacement (μm) | Exact fraction |
|---|---|
| −2 | 1 / 16 |
| −1 | 4 / 16 |
| 0 | 6 / 16 |
| 1 | 4 / 16 |
| 2 | 1 / 16 |
Read the histogram as counts and probabilities
| Interval (μm) | Count | Finite-step probability | Gaussian probability |
|---|---|---|---|
| −2.5 to −1.5 | 125 | 0.0625 | 0.060598 |
| −1.5 to −0.5 | 491 | 0.25 | 0.24173 |
| −0.5 to 0.5 | 762 | 0.375 | 0.38292 |
| 0.5 to 1.5 | 502 | 0.25 | 0.24173 |
| 1.5 to 2.5 | 120 | 0.0625 | 0.060598 |
What remains different after many steps?
| Steps | Sample gap | Law gap | Sample mean square (μm²) | Model mean square (μm²) |
|---|---|---|---|---|
| 4 | 0.192 | 0.1875 | 0.9865 | 1 |
| 16 | 0.104 | 0.09819 | 3.997 | 4 |
| 64 | 0.051462 | 0.049673 | 16.021 | 16 |
| 400 | 0.038411 | 0.019935 | 97.652 | 100 |
A particle jostled by molecules takes many small, independent steps. Whatever the shape of one step, so long as it is symmetric and very large steps are rare enough, the spread after many steps grows as the square root of the time, and its shape comes to look like a bell curve.
Section 4 of the Brownian paper supposes an interval τ short compared with any time we observe, but long enough that a particle's motions in successive intervals are independent, and a law φ(Δ) for the displacement Δ in one interval that is symmetric, φ(Δ) = φ(−Δ), and nonzero only for small Δ. Expanding the new distribution in powers of Δ, symmetry removes the odd terms and the second-order term leaves the diffusion equation ∂f/∂t = D ∂2f/∂x2, with D = (1/τ)∫(Δ2/2)φ(Δ)dΔ. From a point start its solution is the Gaussian law of errors, with root-mean-square displacement λx = √(2Dt). The instrument makes the argument concrete with walkers that step every τ = 0.1 s: coin steps of ±0.5 μm, or uniform or Gaussian steps with the same root-mean-square size. All three give D = (0.5 μm)2/(2 × 0.1 s) = 1.25 μm2/s and the same mean square after n steps, n × 0.25 μm2. What differs is the shape. After 4 coin steps the exact distribution is 1, 4, 6, 4 and 1 sixteenths, whose cumulative probability differs from the Gaussian's by up to 0.1875, and the difference shrinks as the steps add up.
Follow one walker. Every τ = 0.1 s it takes a step Δ: with the coin, +0.5 μm or −0.5 μm, equally likely. After n steps its position is the sum xn = Δ1 + Δ2 + … + Δn. Each step averages to zero, because +0.5 and −0.5 are equally likely, so the average position stays at the start. Now square the sum. It contains the n squared steps, Δ12 + … + Δn2, and cross terms such as 2Δ1Δ2. Each squared coin step is exactly 0.25 μm2. A cross term averages to zero when the steps are independent, since Δ1Δ2 is +0.25 μm2 and −0.25 μm2 equally often. So the average of xn2 is n × 0.25 μm2. After 4 steps, 0.4 s, that is 1 μm2, a root-mean-square distance of 1 μm; the 2000 simulated walkers give 0.9865 μm2 and 0.993 μm. Since t = nτ, the mean square is (0.25 μm2/0.1 s) × t, which is 2Dt with D = 0.25/(2 × 0.1) = 1.25 μm2/s, Einstein's D = (1/τ)∫(Δ2/2)φ(Δ)dΔ written for a coin. For the shape, count paths. Four coin steps make 24 = 16 equally likely paths. The walker ends at +2 μm only if all four steps go right, 1 path; at +1 μm if three do, 4 paths; at 0 if two do, 6 paths; then 4 and 1 on the left. So the chances are 1/16, 4/16, 6/16, 4/16 and 1/16, that is 0.0625, 0.25, 0.375, 0.25 and 0.0625, and the walkers' histogram gives 0.0625, 0.2455, 0.381, 0.251 and 0.06. The Gaussian with the same mean square puts 0.383 in the middle bin and 0.061 in each outer one. Einstein's route goes through the diffusion equation instead. The number of particles at x after one more interval is a sum over every displacement Δ that could bring them there, f(x, t + τ) = ∫f(x + Δ, t)φ(Δ)dΔ. Expand f(x + Δ, t) = f + Δ ∂f/∂x + (Δ2/2) ∂2f/∂x2 + …. The term in Δ averages to zero by symmetry, the constant term gives f back, and what is left is τ ∂f/∂t = (∂2f/∂x2) ∫(Δ2/2)φ(Δ)dΔ, the diffusion equation. Two assumptions carry the weight. With a biased coin that steps right 0.6 of the time, the mean step is 0.6 × 0.5 − 0.4 × 0.5 = 0.1 μm and the crowd drifts at 1 μm/s, a first-order term the argument drops. With Cauchy-shaped steps the variance is infinite, and no finite D exists.
Einstein reaches D through the diffusion equation, not by adding steps: the 1905 paper never writes the mean square of a sum of n steps, and its τ is an interval chosen for the argument, not a tick of the motion. He called the Gaussian result what was to be expected, the law of random errors, and added that the root-mean-square total displacement in three dimensions is λx√3. Smoluchowski reached the square-root law by a kinetic argument in 1906, with a numerical factor differing from Einstein's by 64/27. Pearson named the random walk in a letter to Nature in 1905, and Rayleigh answered from his 1880 work on vibrations of random phase; Bachelier had used the same diffusion equation for prices in 1900. The shape test here, a Kolmogorov distance with a Dvoretzky–Kiefer–Wolfowitz bound on sampling error, is statistics of 1933 and 1956.
Change an assumption, not just a slider
The next three comparisons are analytical. No biased-coin or Cauchy trajectory is drawn by this instrument.
Remove symmetry: biased left/right jumps
With right-step probability 0.6, the mean step is 0.1 μm. Drift speed is 1 μm/s. The centered-variance coefficient is 1.2 μm²/s.
A nonzero mean step produces drift. The pure-diffusion argument omits that first-order term.
Remove finite variance: Cauchy steps
A positive step interval and finite step moments are required; the Cauchy variance is not finite.
That failure belongs to the pure-diffusion argument, not to the existence of a mathematical Cauchy walk. This preview does not simulate that different transport law.
Shrink the interval: what must stay fixed?
Shrinking the interval at fixed step size makes the coefficient grow without bound. A finite diffusion limit instead keeps step variance divided by twice the interval fixed.
| Interval (s) | Keep step fixed: coefficient (μm²/s) | Reduce step RMS to (μm) | Keep ratio fixed: coefficient (μm²/s) |
|---|---|---|---|
| 0.1 | 1.25 | 0.5 | 1.25 |
| 0.01 | 12.5 | 0.15811 | 1.25 |
| 0.001 | 125 | 0.05 | 1.25 |
| 0.0001 | 1250 | 0.015811 | 1.25 |
Model, trial identity, and numerical limits
Independent symmetric steps with finite variance are assumed. The fixed jumps are a mathematical bridge, not a microscopic theory of tracer collisions. Real tracers need a justified coarse-graining time before independence can be assumed. The three step laws are matched by variance, not fourth moment.
Twenty traces and a bounded set of all-walker checkpoints are retained. A cached observation reads its checkpoint; another observation replays identical counter-indexed draws. Neither creates a different realization. This accepted calculation used 800000 random draws, including 0 replayed draws. The full trial identifies 800000 draws and currently retains 144160 bytes.
The work ceiling is five million walker-steps and the private-recording ceiling is eight MiB. The uniform finite-step shape calculation is bounded to 400 observed steps. Its numerical result is not an interval-arithmetic enclosure. Gaussian draws use the host calculation; cross-engine bitwise parity and FrankenSim WASM conformance are not claimed.
These are model calculations, not experimental evidence. The source-aligned critical edition, reviewed historical constants, and full control-tape format remain in preparation.
Show the code
Audited TypeScript reference evaluator: the owner on this device, or the host fallback for a FrankenSim capability.
kernelDiffusivity · src/physics/reference/diffusion/walkLaws.ts · revision workspace · sha256:b2b39a0e609f3ac519ba4b95fd99332d0170518a6bcf48b5e48b444c378eac0b
This is the function that produced the current snapshot.
In words
A symmetric step with finite variance has diffusivity equal to that variance divided by twice the step interval.
Mathematics
Implementation
export function kernelDiffusivity(
kernel: StepKernel,
tau: number,
symmetryTolerance = 1e-12,
): Readonly<{
diffusion: ScientificResult;
drift: ScientificResult;
centeredDiffusion: ScientificResult;
}> {
const m = kernelMoments(kernel);
const bad = (id: string, unit: string, reason: string) =>
outside(id, unit, "kernelDiffusivity", "symmetric-finite-variance", reason);
if (
!Number.isFinite(tau) ||
tau <= 0 ||
m.mean.status !== "value" ||
m.variance.status !== "value" ||
typeof m.mean.value !== "number" ||
typeof m.variance.value !== "number"
) {
const reason =
"A positive step interval and finite step moments are required; the Cauchy variance is not finite.";
return {
diffusion: bad("diffusionCoefficient", "m2/s", reason),
drift: bad("driftVelocity", "m/s", reason),
centeredDiffusion: bad("centeredDiffusionCoefficient", "m2/s", reason),
};
}
const centered = value(
"centeredDiffusionCoefficient",
"m2/s",
"kernelDiffusivity",
m.variance.value / (2 * tau),
m.variance.value > 0,
);
return {
diffusion:
Math.abs(m.mean.value) <= symmetryTolerance
? value(
"diffusionCoefficient",
"m2/s",
"kernelDiffusivity",
m.variance.value / (2 * tau),
m.variance.value > 0,
)
: bad(
"diffusionCoefficient",
"m2/s",
"A nonzero mean step produces drift. The pure-diffusion argument omits that first-order term.",
),
drift: value("driftVelocity", "m/s", "kernelDiffusivity", m.mean.value / tau),
centeredDiffusion: centered,
};
}Audited TypeScript reference evaluator: the owner on this device, or the host fallback for a FrankenSim capability.
randomWalkMoments · src/physics/reference/diffusion/walkLaws.ts · revision workspace · sha256:6783075a2530f6028f515501e415352b59fe2d77d084d759a97af6995880ecb9
This function computes the listed outputs when it runs.
In words
After n independent steps the mean-square displacement is n times the step variance.
Mathematics
Implementation
export function randomWalkMoments(
stepRms: number,
tau: number,
n: number,
): Computation<{
mean: number;
meanSquare: number;
rms: number;
elapsedTime: number;
diffusion: number;
}> {
if (!isCount(n) || !Number.isFinite(stepRms) || stepRms <= 0 || !Number.isFinite(tau) || tau <= 0)
return invalid("Use positive finite step RMS and interval, and 0–10000 steps.");
const meanSquare = n * stepRms * stepRms,
diffusion = (stepRms * stepRms) / (2 * tau),
elapsedTime = n * tau;
if (
![meanSquare, diffusion, elapsedTime].every(Number.isFinite) ||
diffusion <= 0 ||
(n > 0 && (meanSquare === 0 || elapsedTime === 0))
)
return numerical("The moment calculation exceeded binary64 range.");
return {
kind: "accepted",
data: { mean: 0, meanSquare, rms: Math.sqrt(meanSquare), elapsedTime, diffusion },
};
}Audited TypeScript reference evaluator: the owner on this device, or the host fallback for a FrankenSim capability.
coinWalkDistribution · src/physics/reference/diffusion/walkLaws.ts · revision workspace · sha256:feae1213b1fc80d262edcbab8d8110da13a122b91baa5378607cf805ebc98855
This function computes the listed outputs when it runs.
In words
A fair coin walk has an exact binomial distribution on the reachable lattice points.
Mathematics
Implementation
/** Exact integer coefficients through n=64; positive center-out recurrence otherwise.
* Central normalization avoids cancellation and factorial overflow. Extreme tails
* beyond binary64 at large n round to zero; no such tails occur in the n<=400 fixtures.
*/
export function coinWalkDistribution(n: number, ell: number): Computation<CoinDistribution> {
if (!isCount(n) || !Number.isFinite(ell) || ell <= 0 || !Number.isFinite(n * ell))
return invalid("Use 0–10000 steps and a positive finite step scale.");
const positions = Float64Array.from({ length: n + 1 }, (_, k) => (2 * k - n) * ell),
probabilities = new Float64Array(n + 1);
if (n <= 64) {
const coefficients: string[] = [];
const denominator = 1n << BigInt(n);
let coefficient = 1n;
for (let k = 0; k <= n; k++) {
coefficients.push(coefficient.toString());
probabilities[k] = Number(coefficient) / Number(denominator);
if (k < n) coefficient = (coefficient * BigInt(n - k)) / BigInt(k + 1);
}
return {
kind: "accepted",
data: { positions, probabilities, coefficients, denominator: denominator.toString() },
};
}
const mid = Math.floor(n / 2);
probabilities[mid] = 1;
for (let k = mid; k < n; k++) {
const pk = probabilities[k] ?? 0;
probabilities[k + 1] = (pk * (n - k)) / (k + 1);
}
for (let k = mid; k > 0; k--) {
const pk = probabilities[k] ?? 0;
probabilities[k - 1] = (pk * k) / (n - k + 1);
}
let total = 0,
correction = 0;
for (const p of probabilities) {
const y = p - correction,
t = total + y;
correction = t - total - y;
total = t;
}
for (let k = 0; k <= n; k++) {
const pk = probabilities[k] ?? 0;
probabilities[k] = pk / total;
}
return { kind: "accepted", data: { positions, probabilities } };
}Audited TypeScript reference evaluator: the owner on this device, or the host fallback for a FrankenSim capability.
recordWalks · src/physics/reference/diffusion/walks.ts · revision workspace · sha256:d8d45c494c5a564337a3ad369543562ad3d53b207e4cb39113cf70f28a54f64c
This function computes the listed outputs when it runs.
In words
Draw independent walker steps from the chosen kernel and record a bounded set of traces.
Mathematics
Implementation
export async function recordWalks(
input: WalkSetup,
selectedStep: number,
options: WalkExecutionOptions = {},
): Promise<Computation<WalkRecording>> {
const valid = validate(input);
if (valid.kind !== "accepted") return valid;
const p = valid.data;
if (!Number.isInteger(selectedStep) || selectedStep < 0 || selectedStep > p.runSteps)
return invalid("Observe an integer step within the declared recording.");
let config: ReturnType<typeof execution>;
try {
config = execution(options);
} catch {
return invalid("Use a bounded deterministic chunk size.");
}
if (options.cancelled?.()) return cancelled();
const protectedSteps = new Set([
0,
...WALK_MILESTONES.filter((n) => n <= p.runSteps),
p.runSteps,
]);
const checkpoints = new Map(
[...new Set([...protectedSteps, selectedStep])]
.sort((a, b) => a - b)
.map((n) => [n, new Float64Array(p.walkers)]),
);
const traceValues = new Float64Array(Math.min(WALK_TRACE_COUNT, p.walkers) * (p.runSteps + 1));
let work = 0;
for (let walker = 0; walker < p.walkers; walker++) {
const next = sampler(p, walker);
let x = 0;
for (let n = 1; n <= p.runSteps; n++) {
if (work % config.chunk === 0) {
if (options.cancelled?.()) return cancelled();
await config.yieldControl();
if (options.cancelled?.()) return cancelled();
}
x += next();
work++;
if (!Number.isFinite(x))
return failed(
"A walk coordinate exceeded the representable range; no partial trial was accepted.",
);
const checkpoint = checkpoints.get(n);
if (checkpoint) checkpoint[walker] = x;
if (walker < WALK_TRACE_COUNT) traceValues[walker * (p.runSteps + 1) + n] = x;
}
}
if (options.cancelled?.()) return cancelled();
return {
kind: "accepted",
data: Object.freeze({
setup: p,
checkpoints,
traceValues,
protectedSteps,
allocationId: BM05_ALLOCATION.allocationId,
normalVersion: HOST_NORMAL_VERSION,
draws: work * WALK_KERNELS[p.kernel].drawsPerStep,
retainedBytes:
traceValues.byteLength +
[...checkpoints.values()].reduce((sum, a) => sum + a.byteLength, 0),
}),
};
}The explanation
Full explanation
Change the shape of each step while keeping its variance, and compare the spread after many steps. For independent steps the mean square displacement grows in proportion to the number of steps, whatever the shape of a single step.
Show every step of the investigation
Begin with the coin walk you can count exactly, then switch to other step shapes with the same variance. Compare the spread and the shape at several step counts, and check which assumptions the result needs.
An explanatory model, not an observation of nature. This embed starts from the laboratory’s worked defaults, not a saved run. Presentation options change the surrounding guide, never the numerical inputs.