Take Maxwell's four equations at face value. They say an accelerating charge must radiate light — and an electron circling a nucleus is always accelerating. Follow the algebra from Maxwell to the Larmor formula, feed it a hydrogen orbit, and the inescapable result is that the electron spirals into the nucleus in about 16 trillionths of a second. Every step here is correct classical electrodynamics. The catastrophe it predicts is exactly why the world cannot be classical — and why quantum mechanics had to exist.
HONESTY TIER A · DIRECT exact classical electrodynamics — the physics is right; its prediction is wrong, and that is the point
1.6×10⁻¹¹ s
collapse time · from a₀
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radius now · live
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orbit freq · live
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radiated power · live
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revolutions · live
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self-checks
From Maxwell's equations to the falling electron animated
Press Play and step through the chain. Each line lights up as the picture shows what it means — the static fields, light as a travelling wave, the kink an accelerating charge throws off, the Larmor power pattern, the electron's centripetal acceleration, and finally the death spiral. It is all one thread: charges that accelerate must radiate, so a classical orbit cannot last.
static charge & its field
Step 1 / 7
the classical result, at the Bohr radius
τ = 4π²ε₀²m²c³r₀³ / e⁴
The death spiral · classical hydrogen
An electron that radiates cannot keep its orbit
The electron loses energy to radiation every instant, so its orbit shrinks and its whirl speeds up — a chirp that ends in the nucleus. Watch the real numbers: radius in picometres, frequency in petahertz, power in watts, and the clock in trillionths of a second.
Starting radius
Show
The readouts are real SI values from the exact classical law. The number of loops drawn is compressed for visibility — the true count is shown as "revolutions".
Live readout
radiated power (log)—
Radius r(t)=r₀(1−t/τ)^{1/3}; power P=e²a²/6πε₀c³ climbs as 1/r⁴, so the last loops radiate most violently. At r→0 the classical atom is gone.
Starting radius r₀1.00 a₀
Simulation speed1.0×
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Elapsed t / τ0%
Home · First Principles · Why the Classical Atom Collapses
1 · The solved equations of the collapse
The derivation ends in three closed-form results for a classical electron losing energy to Larmor radiation from a Coulomb orbit. Every symbol is a measured constant; plug in the Bohr radius and the numbers are brutal.
How the radius falls
exact · r₀ → 0
$$r(t)=r_0\left(1-\frac{t}{\tau}\right)^{1/3}$$
The orbit shrinks slowly at first, then plunges. Set from \(\dot E=-P\) with \(E=-e^2/8\pi\varepsilon_0 r\). It reaches the nucleus in finite time, not asymptotically.
Scales as \(r_0^{3}\). From the Bohr radius \(a_0=52.9\,\)pm it is 1.56×10⁻¹¹ s — sixteen picoseconds. Hydrogen would not survive a nanosecond.
The frequency chirp
f₀ ≈ 6.6 PHz → ∞
$$f(t)=f_0\left(1-\frac{t}{\tau}\right)^{-1/2}$$
As r shrinks the whirl speeds up without bound, so the emitted light sweeps continuously upward — a smear, not the sharp spectral lines real atoms show.
$$P=\frac{e^{2}a^{2}}{6\pi\varepsilon_0 c^{3}},\qquad a=\frac{e^{2}}{4\pi\varepsilon_0 m r^{2}},\qquad E=-\frac{e^{2}}{8\pi\varepsilon_0 r}$$
Larmor power · Coulomb centripetal acceleration · total energy of a circular orbit — the three inputs to \(\dot E=-P\)
2 · The same physics, at every level
One chain of reasoning, four readings. A curious teenager learns that shaking a charge makes light; a graduate student reads the Liénard–Wiechert radiation field and the Larmor integral. Same Maxwell's equations throughout.
Amiddle school
Wiggle a charge, make light. Electric charges that speed up or change direction send out ripples in the electromagnetic field — that's what light is. An electron going in a circle is always changing direction, so it must be making light and losing energy.
Bhigh school
Radiating costs energy, so the orbit sags. The light carries energy away. Where does it come from? The electron's own motion. As it pays out energy it falls closer to the nucleus and circles faster — a spiral that ends in a crash.
Ccollege
Larmor + Coulomb → a solvable ODE. The Larmor power \(P=e^2a^2/6\pi\varepsilon_0c^3\) with the Coulomb acceleration and \(E=-e^2/8\pi\varepsilon_0 r\) gives \(\dot r\propto -1/r^2\), integrating to \(r(t)=r_0(1-t/\tau)^{1/3}\).
Dgraduate
The 1/r far field is the whole story. The Liénard–Wiechert potentials split into a \(1/r^2\) bound field and a \(1/r\) radiation field \(\propto a_\perp\). Only the latter survives the \(r^2\) of the Poynting sphere — so acceleration, and only acceleration, radiates.
3 · Verification computed live
Each row is evaluated by this page from the CODATA constants and the classical laws, and cross-checked against a known value or a numerical integration. All were reproduced offline in Python to the precision shown.
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Wave speed \(c=1/\sqrt{\mu_0\varepsilon_0}\)
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299 792 458 m/s
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Larmor forms \(\mu_0 q^2a^2/6\pi c = q^2a^2/6\pi\varepsilon_0 c^3\)
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ratio = 1
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Classical orbit energy at a₀ = \(-e^2/8\pi\varepsilon_0 a_0\)
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−13.606 eV (Rydberg)
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Collapse time \(\tau(a_0)\), closed form
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1.56×10⁻¹¹ s
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Numerical \(\dot r=-K/r^2\) fall time vs τ
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agree
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4 · Boundary of validity mandatory
The physics is exact — the conclusion is wrong, and that is the lesson
Honesty tier A (direct): every equation here is textbook classical electrodynamics, and the collapse time is verified in §3. Unlike the rest of the First Principles series, this page's prediction is false — real hydrogen is stable for eternity. The value of the calculation is precisely that it is right in its reasoning and catastrophic in its result: that contradiction is what forced quantum mechanics.
The derivation is correct
Maxwell → wave equation → Liénard–Wiechert radiation field → Larmor power → the collapse ODE are each exact within classical physics. Nothing here is a cheat; the algebra genuinely follows.
valid · classical electrodynamics
The prediction is empirically false
Atoms do not collapse. Hydrogen has sat stable for 13.8 billion years. So one of classical physics' premises must fail at atomic scale — and it does.
contradicted · atoms are stable
What quantum mechanics changes
The electron is not a point on a track. A stationary state is a standing wave of fixed energy with \(\langle\dot{\mathbf p}\rangle\) that does not radiate; only transitions between levels emit the sharp lines we see.
resolution · quantised states
Continuous vs discrete light
The classical chirp predicts a smooth smear of frequencies. Real atoms emit a discrete line spectrum (Balmer, Lyman…). The spectrum alone falsifies the classical picture.
contradicted · line spectra
Non-relativistic, but that's fine
At a₀ the electron moves at \(v\approx0.007c\), so relativistic corrections are tiny and not the reason it "should" collapse. The catastrophe is pure radiation reaction, not speed.
valid · v ≪ c regime
Point charge, no self-force subtlety
We use Larmor's total power, not the full Abraham–Lorentz radiation-reaction force. For this slow inspiral the energy-balance shortcut \(\dot E=-P\) is accurate to the collapse time quoted.
approximation · energy balance
Bottom line. Trust every line of the derivation and the 1.6×10⁻¹¹ s collapse time — they are correct classical physics, verified in §3. Then disbelieve the conclusion, because nature does. The gap between an airtight argument and a stable universe is the doorway to quantum mechanics — see the companion pages Where Classical Physics Breaks and EM & the Atom.
References
Maxwell 1865. A Dynamical Theory of the Electromagnetic Field. Phil. Trans. R. Soc. 155. — the four equations and light as an EM wave.
Larmor 1897. On the theory of the magnetic influence on spectra… Phil. Mag. 44. — the radiated-power formula \(P=q^2a^2/6\pi\varepsilon_0c^3\).
Liénard 1898 / Wiechert 1900. The retarded potentials of a moving point charge — the \(1/r\) radiation field \(\propto a_\perp\).
Rutherford 1911. The scattering of α and β particles… Phil. Mag. 21. — the nuclear atom that classical physics could not stabilise.
Bohr 1913. On the constitution of atoms and molecules. Phil. Mag. 26. — quantised orbits invented to escape the collapse.
Jackson, Classical Electrodynamics 3rd ed., ch. 14 & 16. — Larmor, radiation reaction, and the classical collapse estimate.
Griffiths, Introduction to Electrodynamics, §11.2 & problem on atomic lifetime. — the 1.6×10⁻¹¹ s result derived here.
Feynman Lectures, Vol. I §2, Vol. II §21. — accelerating charges radiate; the intuition behind the far field.