🌌 Astrophysics · General Relativity
📅 March 2026⏱ ~10 min read🔴 Advanced

Gravitational Waves

On 14 September 2015, two L-shaped instruments separated by 3,000 km detected a distortion of spacetime smaller than a proton. The signal lasted 0.2 seconds. It confirmed a prediction of general relativity that Einstein himself doubted could ever be measured.

1. What Are Gravitational Waves?

General relativity describes gravity not as a force but as the curvature of spacetime caused by mass and energy. When massive objects accelerate asymmetrically, the changing curvature propagates outward as waves at the speed of light: gravitational waves.

Unlike electromagnetic waves, gravitational waves stretch and squeeze space itself — alternately elongating space along one axis while compressing it along the perpendicular axis. This is the "plus" (h+) and "cross" (h×) polarizations.

The amplitude — called strain h — measures the fractional change in distance: h = ΔL/L. LIGO measured h ~ 10⁻²¹, meaning a 4 km arm changed by ~10⁻¹⁸ m — 1/1000th the diameter of a proton.

2. The Quadrupole Formula

Einstein's quadrupole formula gives the power radiated as gravitational waves. For a binary system with total mass M, reduced mass μ, and orbital separation a:

Gravitational wave power (quadrupole) P = −32/5 · G⁴/c⁵ · (m₁m₂)²(m₁+m₂) / a⁵

Characteristic strain at distance r:
h ~ (G/c⁴) · (2 · d²I/dt²) / r

where I_ij is the reduced mass quadrupole moment.

Crucially, P ∝ a⁻⁵: as the binary spirals in, it radiates more power, which shrinks the orbit further, which increases the radiation — a runaway inspiral. This is why binary neutron stars merge in finite time (Hulse-Taylor pulsar inspired the 1993 Nobel Prize).

Chirp mass: For a compact binary, the dominant quantity extracted from the waveform is the chirp mass: M_c = (m₁m₂)^(3/5) / (m₁+m₂)^(1/5). It controls how fast the frequency increases (the "chirp"). GW150914 had M_c ≈ 28.3 M☉.

3. How LIGO Works

LIGO (Laser Interferometer Gravitational-Wave Observatory) uses Michelson interferometry with 4 km arms to detect the differential length change caused by a passing wave.

4. Reading the Strain Signal

A binary black hole merger signal has three phases:

Inspiral frequency evolution f_GW = 2 f_orbital
df/dt = (96/5) · π^(8/3) · (G M_c / c³)^(5/3) · f^(11/3)

Template-matched filtering: GR predicts waveform shapes as a function of masses, spins, sky angles. LIGO cross-correlates ~10⁵ precomputed templates against the data. Detection threshold: SNR > 8 in each detector.

5. Key Detections

EventDateTypeMasses (M☉)Distance (Mpc)
GW1509142015-09-14BBH36 + 29 → 62~430
GW1708172017-08-17BNS1.17 + 1.36~40
GW1905212019-05-21BBH85 + 66 → 142~5.3 Gpc
GW2001052020-01-05NSBH8.9 + 1.9~280

As of O3 (third observing run), LIGO/Virgo/KAGRA have catalogued over 90 compact binary merger candidates. GW190521 produced an intermediate-mass black hole (~142 M☉) in the "pair-instability supernova gap" — masses that ordinary stellar evolution cannot produce, suggesting hierarchical mergers.

6. Multi-Messenger Astronomy

GW170817 was historic: the first binary neutron star merger detected in gravitational waves and electromagnetic light, opening the era of multi-messenger astronomy.

7. The Future — LISA & ET

Ground-based detectors hit a frequency floor ~1–10 Hz (seismic noise). Two next-generation instruments push further:

Gravitational wave astronomy: Each bandpass probes different sources. Ground detectors → stellar-mass mergers. Space → supermassive BH mergers. Pulsar arrays → the universe's loudest, oldest sources. Together they map the entire GW sky.