The Four Fundamental Forces

Every phenomenon in the universe — from falling apples to exploding stars — arises from four fundamental interactions. Each has its own carrier, its own range, and its own strength.

G
Gravity
Carrier: graviton (?)
Range∞
Strength10⁻³⁸
Acts oneverything
γ
Electromagnetism
Carrier: photon (γ)
Range∞
Strength10⁻²
Acts oncharge
g
Strong Force
Carrier: 8 gluons
Range~1 fm
Strength1 (strongest)
Acts oncolor charge
W/Z
Weak Force
Carrier: W±, Z⁰
Range~0.001 fm
Strength10⁻⁶
Acts onfermions
Relative strengths compared (normalized to strong force = 1)
Strong
1
Electromag.
10⁻²
Weak
10⁻⁶
Gravity
10⁻³⁸
01 — Gravity

Gravity

The weakest but most universal force. It acts on everything that carries energy, across any distance — and yet it's the only force for which we have no quantum theory.

No QFT framework
Carrier particleGraviton (hypothetical)
Spin2
Carrier mass< 1.2×10⁻²³ eV/c²
Range∞ (1/r²)
Relative strength~10⁻³⁸
Acts onall mass / energy
TheoryGeneral relativity
Graviton detectednone

Gravity is the only one of the four forces that's directly noticeable in everyday life — because it's always attractive and accumulates over cosmic distances. Electromagnetism has just as much reach, but positive and negative charges cancel each other out in matter.

Within the Standard Model, gravity simply cannot be quantized. A spin-2 graviton would be the natural carrier, but the resulting quantum field theories aren't renormalizable — they blow up at high energies. The graviton remains hypothetical; the upper bound on its mass comes from LIGO measurements of gravitational waves.

This is why physicists are searching for a theory of quantum gravity — string theory and loop quantum gravity are the best-known candidates, neither with any experimental support.

m₁ m₂ G (Spin 2) FEYNMAN DIAGRAM
Graviton exchange between two masses
02 — Electromagnetism

Electromagnetism

Light, chemistry, electronics — all electromagnetic. The exchange of massless photons reaches infinitely far and accounts for nearly everything we see and touch in daily life.

QED
Carrier particlePhoton (γ)
Spin1
Carrier mass0
Range∞ (1/r²)
Relative strength~10⁻²
Coupling constantα ≈ 1/137
Acts onelectric charge
TheoryQED

Electromagnetism is described by quantum electrodynamics (QED) — the most precisely tested theory in physics. The electron's magnetic moment matches its predicted value to twelve decimal places.

The carrier particle, the photon, is massless and travels at the speed of light. Like charges repel, unlike charges attract — unlike gravity, electromagnetism can therefore be both attractive and repulsive, which is why it's almost always cancelled out macroscopically in matter.

The fine-structure constant α ≈ 1/137 (dimensionless) measures the strength of the coupling. Its value is one of physics' great open mysteries — no one knows why it takes exactly this value.

e⁻ e⁻ e⁻ e⁻ γ FEYNMAN DIAGRAM
Compton scattering: e⁻e⁻ via photon
03 — Strong Interaction

Strong Force

The strongest force in the universe traps quarks inside protons and neutrons — and holds protons together in the atomic nucleus. It works on a completely different principle from the other forces: quark confinement.

QCD
Carrier particle8 gluons
Spin1
Carrier mass0
Range~1 fm (10⁻¹⁵ m)
Relative strength1 (strongest)
Acts onColor charge (r, g, b)
Special featureConfinement
TheoryQCD (SU(3))

Quarks carry a color charge (red, green, blue — purely symbolic). The eight gluons transmit the strong force between them. Crucially, gluons themselves carry color charge and therefore interact with one another — unlike photons, which carry no electric charge.

This leads to confinement: the farther apart two quarks are pulled, the stronger the force becomes — like a rubber band. Given enough energy, the band snaps, but instead of freeing the quarks, new quark-antiquark pairs form instantly. Free quarks simply don't exist in nature.

At very short distances (very high energies), by contrast, quarks become almost free — asymptotic freedom, for which Gross, Politzer, and Wilczek received the Nobel Prize in 2004.

q (r) q (b) q (g) q (r) g FEYNMAN DIAGRAM
Quark scattering via gluon exchange
04 — Weak Interaction

Weak Force

The weak force is responsible for radioactive beta decay and is the only force that can change particle flavor — and that violates parity. Without it, the sun wouldn't burn.

Electroweak
Carrier particleW⁺, W⁻, Z⁰
Spin1
Mass W±80.4 GeV/c²
Mass Z⁰91.2 GeV/c²
Range~0.001 fm (10⁻¹⁸ m)
Relative strength~10⁻⁶
Acts onall fermions
Special featureParity violation

The carrier particles W± and Z⁰ are extremely massive at over 80 GeV/c² — hence the tiny range (per Heisenberg's uncertainty principle). This mass arises through the Higgs mechanism: the W boson couples to the Higgs field, which gives it its inertia.

Uniquely, the W boson can change particle flavor. In beta-minus decay, a down quark transforms into an up quark: d → u + W⁻. The W⁻ then decays into an electron and an antineutrino. This is how hydrogen is fused into helium in the sun's core.

The weak force violates parity (left-right symmetry) maximally — it couples only to left-handed fermions. This was one of the most surprising discoveries in particle physics (the Wu experiment, 1956).

n p W⁻ e⁻ ν̄e FEYNMAN DIAGRAM
Beta-minus decay: n → p + e⁻ + ν̄e
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