quantity

position

A physical quantity that specifies the location of a particle in space.
21 related articles · 6 formulas

Description

Position is a physical quantity that specifies the location of a particle or object in space relative to a chosen reference frame. In classical mechanics, it is typically represented as a vector (e.g., in Cartesian coordinates: x, y, z) that changes over time. Position is the most fundamental kinematic variable — from it, velocity and acceleration are derived as time derivatives. In quantum mechanics, position becomes an operator, and the concept of a definite trajectory is replaced by a probability distribution.

History

The concept of position as a measurable quantity dates back to ancient Greek geometry and astronomy, but its modern formulation as a vector in a coordinate system was developed by René Descartes in the 17th century (Cartesian coordinates). Newton's laws of motion, published in 1687, formalized the role of position in dynamics.

How it works

Position is defined by a coordinate system and an origin. In three-dimensional space, a position vector r = (x, y, z) gives the displacement from the origin. The time evolution of position is governed by the equations of motion (Newton's laws or the Schrödinger equation in quantum mechanics). In relativity, position is combined with time into a four-dimensional spacetime coordinate, reflecting the fact that simultaneity is frame-dependent.

In practice

Position tracking is essential in GPS navigation, robotics, computer graphics, and particle physics detectors (to reconstruct particle trajectories).

Fun fact

In quantum mechanics, the position of a particle cannot be known with arbitrary precision simultaneously with its momentum, due to the Heisenberg uncertainty principle.

Concept graph →

Formulas

$$V(z) = \phi - eFz - \frac{e^2}{4\pi\epsilon_0 z}$$
Potential energy for electron emission including work function and field.
What is in the formula
Vvariablepotential energy of electron — potential energy joule
zvariabledistance from the metal surface — position metre
φvariablework function of the metal — work function joule
Fvariableapplied electric field strength — electric field volt per metre
econstantcharge of a single proton — elementary charge = 1.602176634e-19 coulomb
ε0constantability of vacuum to permit electric field lines — vacuum permittivity = 8.8541878128e-12 farad per metre
$$T \approx \exp\left(-2\int_{z_1}^{z_2} \sqrt{\frac{2m}{\hbar^2}(V(z)-E)}\, dz\right)$$
Approximate quantum tunneling probability through a barrier.
What is in the formula
Tvariabletunneling probability — transmission probability
z1variableleft turning point of the barrier — position metre
z2variableright turning point of the barrier — position metre
mvariablemass of the tunneling particle — mass kilogram
Vvariablepotential energy as a function of position — potential energy joule
Evariableenergy of the particle — energy joule
ħconstantfundamental quantum of action divided by 2π — reduced planck constant = 1.054571817e-34 joule second
∫operatorsums the integrand over the interval — integral
√operatortakes the non-negative root — square root
expoperatorraises e to the given power — exponential
$$\delta = \int |W(X,P)|\, dX dP - 1$$
Measures nonclassicality via Wigner function negativity.
What is in the formula
WvariableWigner function of the quantum state — Wigner function
Xvariableposition quadrature variable — position metre
Pvariablemomentum quadrature variable — momentum kilogram metre per second
∫ dX dPoperatorintegration over the full phase space — double integral
| |operatorabsolute value of the Wigner function — absolute value
$$\frac{d^2\psi}{dx^2} + \left(k^2 - V(x)\right) \psi = 0$$
Wave equation with potential barrier in quantum mechanics.
What is in the formula
\psivariablewave function — wave function
xvariableposition coordinate — position metre
kvariablewave number — wave number per metre
V(x)variablepotential function — potential energy joule
\frac{d^2}{dx^2}operatorsecond derivative with respect to position — second derivative
$$-\frac{d^2 \psi}{dx^2} + V(x) \psi = E \psi$$
A wave function's evolution in a potential is governed by the Schrödinger equation.
What is in the formula
ψvariablewave function — wave function
xvariableposition coordinate — position metre
V(x)variablepotential energy function — potential energy joule
Evariableenergy eigenvalue — energy joule
d²/dx²operatorsecond derivative with respect to position — second derivative
$$V = \frac{1}{\sqrt{f}} \frac{d^2 \sqrt{f}}{dx^2}$$
An effective potential is defined from a function's second derivative.
What is in the formula
Vvariableeffective potential — potential energy joule
fvariablefunction whose curvature defines the potential
xvariableindependent variable — position metre
d²/dx²operatorsecond derivative with respect to x — second derivative

Related articles · 21

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