Virtual laboratory/Physics/Atomic physics/Heisenberg's uncertainty principle

Heisenberg's uncertainty principle

Tighten the precision of the position measurement. You cannot know a particle's position and momentum precisely at the same time: Δx·Δp ≥ ℏ/2; the smaller Δx, the larger the momentum uncertainty Δp.

Heisenberg's uncertainty principle
Physics · Atomic physics · Heisenberg uncertainty principle (FIZ.ATOM.PP.07)
Position-measurement precision Δx\Delta x1.00 nm
The more precisely we know the particle’s position, the more precisely we know its momentum…
precision Δx
1.00 nm
uncertainty Δp
0.53
product Δx·Δp
0.527
limit ℏ/2
0.527
🎯 Challenge: hit the momentum spread
streak: 0

I’ll give you a target momentum uncertainty Δp — set the position precision Δx so you reach it. Δx·Δp = ℏ/2.

What just happened?

You narrowed the particle’s position region, and its momentum distribution spread out. Position and momentum cannot both be known arbitrarily precisely at the same time — you buy one at the cost of the other.

Heisenberg uncertainty principle:

Δx⋅Δp  ≥  ℏ2\Delta x \cdot \Delta p \;\ge\; \dfrac{\hbar}{2}

— the product of the position uncertainty Δx\Delta x and the momentum uncertainty Δp\Delta p cannot be smaller than ℏ/2\hbar/2. This is not a flaw of the instruments — it is a fundamental feature of nature. ℏ\hbar is the reduced Planck constant.

What does it mean in practice?

The more precisely you measure the position (smaller Δx\Delta x), the larger the momentum uncertainty becomes:

Δp  ≥  ℏ2 Δx\Delta p \;\ge\; \dfrac{\hbar}{2\,\Delta x}

That is why the cloud of points narrows while the momentum distribution grows wide — the product stays under the constant control of the lower limit ℏ/2\hbar/2.

Why don’t we see this in everyday life?

ℏ\hbar is tiny (ℏ≈1.05⋅10−34\hbar \approx 1{.}05\cdot 10^{-34} J·s), so for a ball or a car the imposed spread is immeasurably small. The principle governs the world of electrons, atoms and particles — not macroscopic bodies.

Why you need this for the exam:

Knowing Δx⋅Δp≥ℏ/2\Delta x\cdot\Delta p \ge \hbar/2 lets you estimate the minimum momentum uncertainty (and hence energy) of a confined particle and explain why an electron does not “fall” onto the nucleus. The trick: when you decrease Δx\Delta x, the quantity Δp\Delta p immediately grows — the product stays at the bottom.

Remember

You cannot measure position and momentum perfectly precisely at the same time: Δx⋅Δp≥ℏ/2\Delta x\cdot\Delta p \ge \hbar/2. A more precise position = a more blurred momentum. This is a limit imposed by nature itself, not by the instruments.

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Theory & formulas

The Heisenberg principle

You cannot know a particle's position and momentum precisely at the same time: Δx⋅Δp≥ℏ2\Delta x\cdot\Delta p \ge \dfrac{\hbar}{2} The smaller Δx\Delta x (the better we know the position), the larger Δp\Delta p (the worse we know the momentum).

This is not a measurement error

It is a fundamental feature of the quantum nature of matter, not an imperfection of the instruments. There is also an energy–time relation: ΔE⋅Δt≥ℏ2\Delta E\cdot\Delta t \ge \dfrac{\hbar}{2}.

Notation: Δx\Delta x — position uncertainty, Δp\Delta p — momentum uncertainty, ℏ\hbar — reduced Planck constant, ΔE,Δt\Delta E,\Delta t — energy and time uncertainties.

Frequently asked questions

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What does the uncertainty principle say?

You cannot simultaneously measure a particle's position and momentum precisely (Δx·Δp ≥ ℏ/2).

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What happens when we know the position precisely?

The momentum uncertainty grows — we know it less precisely.

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Is it a measurement error?

No — it is a fundamental property of the quantum nature of matter, not a matter of instruments.

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