quantity

distance

A measure of how far away an object is, affecting the observed signal strength.
8 related articles · 6 formulas

Description

Distance is a fundamental measure of spatial separation between two points, and in physics it underpins the inverse-square law, which dictates that the intensity of a signal (light, sound, gravity) decreases with the square of the distance from its source. This principle is crucial for astronomical measurements, where determining how far away an object is allows scientists to infer its intrinsic luminosity, mass, or velocity. In quantum sensing, distance affects the coupling strength between a sensor and the target signal, with closer proximity yielding stronger interactions and better sensitivity.

History

The concept of distance has been central to physics since antiquity, but its precise astronomical measurement began with the first stellar parallax in 1838 by Friedrich Bessel. The inverse-square law for light was formulated by Johannes Kepler in the 17th century and later refined by Isaac Newton.

How it works

In practice, distance is often measured indirectly through observable effects. For example, the apparent brightness of a known light source (a 'standard candle') reveals its distance via the inverse-square law. Alternatively, parallax — the apparent shift in position of a nearby object against distant background stars as the Earth orbits the Sun — provides a geometric distance. In quantum sensors, the distance to a target is encoded in the strength of the interaction, such as the magnetic dipole coupling, which falls off as the cube of the distance, allowing precise localization of nearby objects.

In practice

Distance measurement is used in LIDAR for autonomous vehicles, in astronomical surveys to map the universe, and in quantum sensing to localize single spins or nanoparticles with nanometer resolution.

Fun fact

The human eye can detect a single photon, but the distance to a star is so vast that the light arriving from it is often less than one photon per second per square centimeter of telescope aperture.

Concept graph →

Formulas

$$V(r) = -g \frac{e^{-r/\lambda}}{r}$$
Potential decaying exponentially with distance.
What is in the formula
VvariablePotential energy — potential energy joule
rvariableRadial distance from source — distance metre
gvariableCoupling strength (not a universal constant) joule metre
λvariableScreening length (range of interaction) — length metre
$$v = H d$$
Recessional velocity of galaxies is proportional to their distance.
What is in the formula
vvariableRecessional velocity of a galaxy — velocity metre per second
HvariableHubble parameter (time-dependent) — hubble parameter per second
dvariableProper distance to the galaxy — distance metre
$$k(r) = rac{\sigma^2 2^{1-\nu}}{\Gamma(\nu)} \left( \frac{\sqrt{2\nu} r}{l} \right)^\nu K_\nu \left( \frac{\sqrt{2\nu} r}{l} \right)$$
A covariance function for Gaussian processes with smoothness parameter ν.
What is in the formula
rvariabledistance between two points — distance metre
νvariablesmoothness parameter
lvariablelength scale parameter — length metre
σvariablevariance amplitude — variance square metre
ΓoperatorGamma function, generalizes factorial — gamma function
K_νoperatorModified Bessel function of the second kind of order ν — modified bessel function second kind
$$h_{ij}^{\text{TT}} = \frac{2G}{c^4 D} \frac{d^2 I_{ij}}{dt^2}$$
Gravitational wave strain from mass quadrupole moment.
What is in the formula
h_{ij}^{\text{TT}}variableTransverse-traceless gravitational wave strain tensor — gravitational wave strain
DvariableDistance from source to observer — distance metre
I_{ij}variableMass quadrupole moment tensor — mass quadrupole moment kilogram metre squared
tvariableTime — time second
GconstantConstant of gravitation in Newton's law — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
cconstantUniversal speed limit and speed of light in vacuum — speed of light = 299792458 metre per second
d^2/dt^2operatorSecond derivative with respect to time — second time derivative
$$F = -\frac{GMm}{r^2} - \frac{4\pi}{3} G m r \rho (1+3w)$$
Gravitational force modified by dark energy pressure, vanishes at w=-1/3.
What is in the formula
FvariableGravitational force magnitude — force newton
MvariableMass of the central object — mass kilogram
mvariableMass of the test particle — mass kilogram
rvariableDistance between masses — distance metre
ρvariableEnergy density of the cosmic fluid — energy density joule per cubic metre
wvariableEquation-of-state parameter of the fluid — equation of state parameter
GconstantUniversal constant of gravitation — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
$$d = \sqrt{(x_1 - x_0)^2 + (y_1 - y_0)^2}$$
Euclidean distance measures straight-line distance between two points.
What is in the formula
dvariableEuclidean distance — distance metre
x₁variablex-coordinate of point 1 — coordinate metre
x₀variablex-coordinate of point 0 — coordinate metre
y₁variabley-coordinate of point 1 — coordinate metre
y₀variabley-coordinate of point 0 — coordinate metre
√operatortakes the square root of the sum — square root

Related articles · 8

Gravitational Noise: How Ripples in Space Erase Quantum Superpositions
Two massive bodies frozen in a quantum superposition resemble a pair of dancers trying to keep a single rhythm while an orchestra blares around them. Each gravitational wave is a musician throwing them off beat.
Cosmology2026-08-062 minarXiv:2608.06247
A Tailwind for Six Runners: How Peculiar Velocities Skewed the Hubble Constant
Six runners sprint down the track, and officials time their speed without noticing a tailwind. The wind blows at their backs, and the stopwatches show a better result than the truth. Roughly this is how six megamasers — natural cosmic lasers in distant galaxies — misled astronomers measuring the expansion rate of the universe.
Quantum Physics2026-08-052 minarXiv:2608.04876express
A Quantum Compass for 3D Vision
A camera looks at two distant sparks. They're so close together that they merge into a single fuzzy blob. It seems impossible to tell them apart — the classic limit of optical microscopy has been reached. But quantum mechanics hints that the light field still holds a secret about where each spark sits.
Instrumentation2026-04-101 minarXiv:2604.09787express
One Galaxy, Two Telescopes: How to Separate Physics from Distortions
If you photograph the same mountain with a film camera and a modern smartphone, you get different images: colors are brighter in one, details are blurrier in the other. The same goes for telescopes: each instrument sees the sky in its own way, adding its own distortions to the true light of galaxies, like a filter through which we look.
Atomic Physics2026-03-241 minarXiv:2603.22981express
All Atoms Fall Alike: A Cosmic Verdict
Galileo, legend has it, dropped balls from the Tower of Pisa to prove that heavy and light objects fall equally. This law formed the foundation of Einstein's theory of gravity. Today, scientists have turned an entire space station into such a tower.
Quantum Physics2026-02-201 minarXiv:2602.18524express
The Clocks That Throw Off the Scales
Ultra-precise scales that catch the slightest changes in gravity work like a keen ear: they hear even the whisper of distant underground voids or the tremors of the Earth's crust. But such instruments have a hidden enemy: their own internal clocks. Time inside the sensor also jitters, and this jitter smears the picture.
Quantum Measurement as a Deformation of Perception: The Bloch Sphere and the Birth of Categories
Quantum mechanics gave us a captivating image: a system’s state is not a frozen point but a wave of possibilities, dancing in an abstract space. Thanks to the work of Шрёдингера and Дирака, we represent it as vectors in Hilbert space.
math.NA2023-08-082 minarXiv:2308.04167
A Gravitational Portrait of Earth from 500 Kilometers Up
Setting up an orchestra without a conductor: the algorithm itself decides which instruments (basis functions) and at what volume (weights) should play to reproduce Earth's gravitational symphony.