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Physics

Essential Physics Equations

Explore foundational physics equations, grouped by domain, with explanations, symbol definitions, SI units, constant values, and the conditions in which they apply.

Classical mechanics

How forces change motion, how energy is transferred, and why momentum is conserved.

Newton’s second law

∑F=ma\sum \mathbf{F} = m\mathbf{a}

The combined force on an object determines its acceleration. A larger mass needs a larger net force to produce the same acceleration. Forces and acceleration have direction, so forces that oppose each other must be combined as vectors. OpenStax · Newton’s second law

Newton’s second law: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
∑F\sum \mathbf{F}Net external forceN\mathrm{N}—
mmMasskg\mathrm{kg}—
a\mathbf{a}Accelerationm s−2\mathrm{m\,s^{-2}}—

When it applies: This form assumes constant mass and an inertial reference frame. Use it for motion much slower than light.

Conservation of linear momentum

∑ipi,initial=∑ipi,final\sum_i \mathbf{p}_{i,\mathrm{initial}} = \sum_i \mathbf{p}_{i,\mathrm{final}}

Objects can exchange momentum during a collision, but their total momentum stays the same when no net external impulse acts on the system. This lets us connect motion before and after a collision without knowing every detail of the impact. OpenStax · Conservation of linear momentum

Conservation of linear momentum: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
pi\mathbf{p}_iMomentum of the ith object; classically, its mass multiplied by its velocitykg m s−1\mathrm{kg\,m\,s^{-1}}—
∑i\sum_iVector sum over all objects in the chosen system——

When it applies: Choose a system with no mass crossing its boundary and negligible net external impulse during the interval. Kinetic energy need not be conserved.

Kinetic energy

K=12mv2K = \frac{1}{2}mv^2

Kinetic energy is the energy associated with motion. Doubling the speed gives four times the kinetic energy at the same mass. That is why stopping a fast vehicle requires much more energy to be removed than stopping a slow one. OpenStax · Kinetic energy

Kinetic energy: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
KKTranslational kinetic energyJ\mathrm{J}—
mmMasskg\mathrm{kg}—
vvSpeed in the chosen reference framem s−1\mathrm{m\,s^{-1}}—

When it applies: This is the nonrelativistic expression for translational motion. Rotation has its own kinetic energy, and speeds near light require a relativistic expression.

Work–energy theorem

Wnet=ΔKW_{\mathrm{net}} = \Delta K

The total work done on a particle equals its change in kinetic energy. Positive net work speeds it up; negative net work slows it down. Work counts the part of a force acting along the displacement, rather than force alone. OpenStax · Work–energy theorem

Work–energy theorem: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
WnetW_{\mathrm{net}}Work done by all forces along the pathJ\mathrm{J}—
ΔK\Delta KFinal kinetic energy minus initial kinetic energyJ\mathrm{J}—

When it applies: Use the particle model in classical mechanics. For an extended or deforming system, also account for rotation, internal energy, and how the system boundary is chosen.

Newton’s law of gravitation

F=Gm1m2r2F = G\frac{m_1m_2}{r^2}

Two masses attract each other with a force that weakens with the square of their separation. The same relationship describes falling objects and much of planetary motion. The force points along the line joining the two masses. OpenStax · Universal gravitation

Newton’s law of gravitation: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
FFMagnitude of the attractive forceN\mathrm{N}—
GGNewtonian gravitational constantm3 kg−1 s−2\mathrm{m^3\,kg^{-1}\,s^{-2}}≈6.67430×10−11\approx 6.67430\times10^{-11}
m1, m2m_1,\ m_2The two masseskg\mathrm{kg}—
rrDistance between the masses’ centresm\mathrm{m}—

When it applies: Applies directly to point masses or nonoverlapping spherically symmetric bodies. Strong gravity and relativistic motion require general relativity.

Oscillations, waves, and optics

Repeating motion, the propagation of disturbances, and the bending of light.

Simple harmonic motion

d2xdt2=−ω2x\frac{d^2x}{dt^2} = -\omega^2 x

Acceleration always points toward equilibrium and is proportional to the displacement. This produces sinusoidal motion, such as an ideal mass on a spring. The negative sign expresses the restoring direction. OpenStax · Simple harmonic motion

Simple harmonic motion: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
xxDisplacement from equilibriumm\mathrm{m}—
ttTimes\mathrm{s}—
ω\omegaAngular frequencyrad s−1\mathrm{rad\,s^{-1}}—
d2x/dt2d^2x/dt^2Second time derivative of displacement: accelerationm s−2\mathrm{m\,s^{-2}}—

When it applies: Assumes a linear restoring force with no damping or driving. Pendulums approximate this motion only for small angles.

Wave speed, frequency, and wavelength

vphase=fλv_{\mathrm{phase}} = f\lambda

A wave crest travels one wavelength during one cycle. Multiplying the number of cycles per second by the distance per cycle gives the crest’s speed. The relationship connects the spatial and temporal patterns of a periodic wave. OpenStax · Mathematics of waves

Wave speed, frequency, and wavelength: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
vphasev_{\mathrm{phase}}Phase speedm s−1\mathrm{m\,s^{-1}}—
ffFrequencyHz\mathrm{Hz}—
λ\lambdaWavelengthm\mathrm{m}—

When it applies: Describes a periodic wave. In a dispersive medium, phase speed can differ from the speed of a wave packet or signal.

Snell’s law of refraction

n1sin⁡θ1=n2sin⁡θ2n_1\sin\theta_1 = n_2\sin\theta_2

Light changes direction when it crosses between materials with different refractive indices. Entering a material with a higher index bends the ray toward the surface normal. The law is used to understand lenses and light passing through water or glass. OpenStax · Refraction

Snell’s law of refraction: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
n1, n2n_1,\ n_2Refractive indices of the incident and transmitted media11—
θ1, θ2\theta_1,\ \theta_2Incident and refracted angles, both measured from the surface normalrad\mathrm{rad}—

When it applies: Use for refraction at an interface between ordinary isotropic media. Some incident angles from a higher-index medium produce total internal reflection instead of a transmitted ray.

Electromagnetism

Charges, currents, and fields. The four Maxwell equations below connect electricity, magnetism, and light.

Coulomb’s law

F=14πε0∣q1q2∣r2F = \frac{1}{4\pi\varepsilon_0}\frac{|q_1q_2|}{r^2}

Electric charges exert forces on each other. Like signs repel and opposite signs attract. The displayed equation gives the force magnitude; its direction lies along the line joining the charges. OpenStax · Coulomb’s law

Coulomb’s law: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
FFElectric force magnitudeN\mathrm{N}—
q1, q2q_1,\ q_2Electric chargesC\mathrm{C}—
rrSeparationm\mathrm{m}—
ε0\varepsilon_0Vacuum permittivityF m−1\mathrm{F\,m^{-1}}≈8.8541878188×10−12\approx 8.8541878188\times10^{-12}
π\piRatio of a circle’s circumference to its diameter11≈3.141592653589793\approx 3.141592653589793

When it applies: This is the electrostatic force between point charges in vacuum. For many charges, add their force vectors; material media require additional treatment.

Lorentz force

F=q(E+v×B)\mathbf{F} = q\left(\mathbf{E} + \mathbf{v}\times\mathbf{B}\right)

Electric and magnetic fields act on a charged particle. The electric part can change its speed. The magnetic part is perpendicular to its velocity, so by itself it changes direction without doing work. OpenStax · Maxwell equations and the Lorentz force

Lorentz force: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
F\mathbf{F}Electromagnetic forceN\mathrm{N}—
qqParticle chargeC\mathrm{C}—
E\mathbf{E}Electric field at the particleV m−1\mathrm{V\,m^{-1}}—
B\mathbf{B}Magnetic field at the particleT\mathrm{T}—
v\mathbf{v}Particle velocity; the cross denotes a vector cross productm s−1\mathrm{m\,s^{-1}}—

When it applies: Fields and velocity must be measured in the same inertial frame. Treat the particle as a point charge and exclude its own field from the applied fields.

Gauss’s law for electricity

∯SE⋅dA=Qencε0\oiint_S \mathbf{E}\cdot d\mathbf{A} = \frac{Q_{\mathrm{enc}}}{\varepsilon_0}

The net electric flux through a closed surface measures the charge enclosed by it. Charges outside the surface affect the field but contribute no net flux through that surface. Symmetry can make this a powerful way to find electric fields. OpenStax · Gauss’s law

Gauss’s law for electricity: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
E\mathbf{E}Electric fieldV m−1\mathrm{V\,m^{-1}}—
SSClosed surface of integration——
dAd\mathbf{A}Outward-pointing area elementm2\mathrm{m^2}—
QencQ_{\mathrm{enc}}Net enclosed chargeC\mathrm{C}—
ε0\varepsilon_0Vacuum permittivityF m−1\mathrm{F\,m^{-1}}≈8.8541878188×10−12\approx 8.8541878188\times10^{-12}

When it applies: One of Maxwell’s equations in SI units, using total charge and the electric field. It does not require a symmetric surface to be valid.

Gauss’s law for magnetism

∯SB⋅dA=0\oiint_S \mathbf{B}\cdot d\mathbf{A} = 0

A closed surface has no net magnetic flux. Magnetic field lines have no isolated sources or sinks in ordinary electromagnetism. Cutting a bar magnet creates smaller magnets, each with both poles, rather than separating the poles. OpenStax · Magnetic fields and lines

Gauss’s law for magnetism: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
B\mathbf{B}Magnetic fieldT\mathrm{T}—
SSClosed surface of integration——
dAd\mathbf{A}Outward-pointing area elementm2\mathrm{m^2}—
∯S\oiint_SIntegral summing the normal component of the field over the closed surface——

When it applies: The Maxwell equation for a theory without magnetic monopoles. Zero net flux does not mean the magnetic field vanishes everywhere on the surface.

Faraday’s law of induction

∮CE⋅dℓ=−dΦBdt\oint_C \mathbf{E}\cdot d\boldsymbol{\ell} = -\frac{d\Phi_B}{dt}

A changing magnetic flux produces a circulating electric field. This is the basis of transformers and induction. The negative sign records Lenz’s law: the induced response opposes the change in flux. OpenStax · Induced electric fields

Faraday’s law of induction: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
E\mathbf{E}Electric fieldV m−1\mathrm{V\,m^{-1}}—
CCClosed loop of integration——
dℓd\boldsymbol{\ell}Directed line element along the loopm\mathrm{m}—
ΦB\Phi_BMagnetic flux through a surface bounded by the loopWb\mathrm{Wb}—
ttTime; the loop integral is the induced electromotive forces\mathrm{s}—

When it applies: This field form uses a stationary loop with consistent loop and surface orientations. Moving conductors also require the magnetic force contribution to electromotive force.

Ampère–Maxwell law

∮CB⋅dℓ=μ0Ienc+μ0ε0dΦEdt\oint_C \mathbf{B}\cdot d\boldsymbol{\ell} = \mu_0 I_{\mathrm{enc}} + \mu_0\varepsilon_0\frac{d\Phi_E}{dt}

Magnetic circulation comes from electric current and changing electric flux. Maxwell’s added flux term makes the law work across a charging capacitor and helps explain how electromagnetic waves propagate. OpenStax · Maxwell’s correction to Ampère’s law

Ampère–Maxwell law: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
B\mathbf{B}Magnetic fieldT\mathrm{T}—
CCClosed loop of integration——
dℓd\boldsymbol{\ell}Directed line element along the loopm\mathrm{m}—
IencI_{\mathrm{enc}}Current through a surface bounded by the loopA\mathrm{A}—
ΦE\Phi_EElectric flux through that surfaceV m\mathrm{V\,m}—
ttTimes\mathrm{s}—
μ0\mu_0Vacuum permeabilityN A−2\mathrm{N\,A^{-2}}≈1.25663706127×10−6\approx 1.25663706127\times10^{-6}
ε0\varepsilon_0Vacuum permittivityF m−1\mathrm{F\,m^{-1}}≈8.8541878188×10−12\approx 8.8541878188\times10^{-12}

When it applies: SI field form for a fixed loop and surface, using total current. Loop direction, surface normal, current, and flux signs follow the right-hand rule.

Ohm’s law

V=IRV = IR

Across an ohmic component, the voltage is proportional to the current. Resistance sets how much voltage is needed for a given current, making this a starting point for analysing resistor circuits. OpenStax · Ohm’s law

Ohm’s law: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
VVPotential difference across the componentV\mathrm{V}—
IICurrent through the componentA\mathrm{A}—
RRResistanceΩ\mathrm{\Omega}—

When it applies: Resistance must be effectively constant under the operating conditions. Diodes, lamps with changing temperature, and many other components are not ohmic.

Thermodynamics and statistical physics

Heat, work, temperature, and the connection between microscopic states and macroscopic behaviour.

Ideal gas law

PV=nRTPV = nRT

Pressure, volume, and temperature are linked for a fixed amount of ideal gas. Heating a sealed, rigid container raises its pressure; allowing expansion can instead increase its volume. The relationship is a model of many particles moving and colliding. OpenStax · Molecular model of an ideal gas

Ideal gas law: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
PPAbsolute pressurePa\mathrm{Pa}—
VVVolumem3\mathrm{m^3}—
nnAmount of gasmol\mathrm{mol}—
RRMolar gas constantJ mol−1 K−1\mathrm{J\,mol^{-1}\,K^{-1}}8.314462618153248.31446261815324
TTAbsolute temperatureK\mathrm{K}—

When it applies: Assumes negligible particle volume and interactions apart from elastic collisions. Real gases approximate it best at low density and away from condensation.

First law of thermodynamics

ΔU=Q−W\Delta U = Q - W

Energy entering a system as heat can increase its internal energy or leave as work. The first law is an energy balance: heat and work are ways to transfer energy, while internal energy belongs to the system’s state. OpenStax · First law of thermodynamics

First law of thermodynamics: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
ΔU\Delta UChange in internal energyJ\mathrm{J}—
QQHeat transferred into the system, positive inwardJ\mathrm{J}—
WWWork done by the system on its surroundings, positive outwardJ\mathrm{J}—

When it applies: This form assumes a closed system with negligible changes in bulk kinetic and gravitational potential energy. A convention that counts work done on the system reverses the work sign.

Second law of thermodynamics

ΔSisolated≥0\Delta S_{\mathrm{isolated}} \geq 0

The total entropy of an isolated system cannot decrease in a macroscopic thermodynamic process. This gives processes a preferred direction: heat spontaneously flows from hotter to colder bodies, and dissipated energy cannot all be recovered as useful work in a cycle. OpenStax · Entropy and the second law

Second law of thermodynamics: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
ΔSisolated\Delta S_{\mathrm{isolated}}Total entropy change of the isolated systemJ K−1\mathrm{J\,K^{-1}}—
≥0\geq 0Zero for a reversible process; positive for an irreversible process——

When it applies: Include the surroundings if the chosen subsystem exchanges heat or matter. A subsystem’s entropy can decrease while total entropy increases.

Boltzmann’s entropy formula

S=kBln⁡ΩS = k_{\mathrm{B}}\ln\Omega

A macroscopic state can be realised by many microscopic arrangements. Entropy measures the logarithm of their number. A state compatible with more microscopic arrangements is more likely when those arrangements are equally probable. OpenStax · Entropy on a microscopic scale

Boltzmann’s entropy formula: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
SSEntropyJ K−1\mathrm{J\,K^{-1}}—
kBk_{\mathrm{B}}Boltzmann constantJ K−1\mathrm{J\,K^{-1}}1.380649×10−231.380649\times10^{-23}
Ω\OmegaNumber of accessible microstates compatible with the macrostate11—
ln⁡\lnNatural logarithm——

When it applies: This counting form assumes equally probable accessible microstates. Unequal probabilities require the more general statistical entropy expression.

Relativity and spacetime

The relationship between mass and energy, the dependence of elapsed time on motion, and gravity as spacetime geometry.

Mass–energy equivalence

E0=mc2E_0 = mc^2

An object has rest energy even when it is not moving. Mass and rest energy are two ways to describe the same physical property. In a nuclear reaction, the difference between initial and final rest masses accounts for energy released; ordinary matter does not readily release all its rest energy. OpenStax · Rest energy and relativistic energy

Mass–energy equivalence: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
E0E_0Rest energyJ\mathrm{J}—
mmInvariant mass, also called rest masskg\mathrm{kg}—
ccSpeed of light in vacuumm s−1\mathrm{m\,s^{-1}}299 792 458299\,792\,458

When it applies: Gives rest energy, not the total energy of a moving object. For a composite system, internal motion and binding energy contribute to its invariant mass.

Relativistic energy–momentum relation

E2=p2c2+m2c4E^2 = p^2c^2 + m^2c^4

Total energy contains both rest energy and the contribution associated with momentum. The relation also applies to massless particles: a photon has energy and momentum even though it has no rest mass. OpenStax · Energy and momentum in relativity

Relativistic energy–momentum relation: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
EETotal energy in the chosen inertial frameJ\mathrm{J}—
ppMagnitude of momentum in that framekg m s−1\mathrm{kg\,m\,s^{-1}}—
mmInvariant masskg\mathrm{kg}—
ccSpeed of light in vacuumm s−1\mathrm{m\,s^{-1}}299 792 458299\,792\,458

When it applies: A special-relativistic relation for a free particle or a system’s total energy, total momentum, and invariant mass. It does not treat mass as increasing with speed.

Time dilation

Δt=Δτ1−v2/c2\Delta t = \frac{\Delta\tau}{\sqrt{1-v^2/c^2}}

A moving clock accumulates less time between two events than the coordinate time assigned by an observer in an inertial frame. The difference is tiny at everyday speeds but measurable for fast particles and precision clocks. OpenStax · Time dilation

Time dilation: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
Δt\Delta tElapsed coordinate time in the observer’s inertial frames\mathrm{s}—
Δτ\Delta\tauProper time measured by the moving clock between the same eventss\mathrm{s}—
vvClock’s speed relative to the observerm s−1\mathrm{m\,s^{-1}}—
ccSpeed of light in vacuumm s−1\mathrm{m\,s^{-1}}299 792 458299\,792\,458

When it applies: This form assumes constant relative speed below light speed in flat spacetime. Varying motion requires integration, and gravity introduces additional time effects.

Einstein’s field equations

Gμν+Λgμν=8πGc4TμνG_{\mu\nu} + \Lambda g_{\mu\nu} = \frac{8\pi G}{c^4}T_{\mu\nu}

Spacetime geometry is linked to the distribution of energy, momentum, and stress. These equations underpin the description of black holes, gravitational waves, and cosmic expansion. The compact notation represents a coupled set of equations rather than a single arithmetic formula. Sean Carroll · Field equations and the cosmological constant

Einstein’s field equations: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
GμνG_{\mu\nu}Einstein tensor, built from spacetime curvaturem−2\mathrm{m^{-2}}—
gμνg_{\mu\nu}Metric tensor, describing spacetime intervals11—
Λ\LambdaCosmological constantm−2\mathrm{m^{-2}}—
TμνT_{\mu\nu}Stress–energy tensor, describing energy, momentum, and stressesJ m−3\mathrm{J\,m^{-3}}—
GGNewtonian gravitational constantm3 kg−1 s−2\mathrm{m^3\,kg^{-1}\,s^{-2}}≈6.67430×10−11\approx 6.67430\times10^{-11}
ccSpeed of light in vacuumm s−1\mathrm{m\,s^{-1}}299 792 458299\,792\,458
μ, ν\mu,\ \nuIndices labelling spacetime components——
π\piRatio of a circle’s circumference to its diameter11≈3.141592653589793\approx 3.141592653589793

Tensor units assume coordinates measured in metres, including light speed multiplied by time for the time coordinate, and a dimensionless metric. Other coordinate conventions can change component units. The cosmological constant is model-dependent, with no universal numerical value.

When it applies: The classical theory of gravity, written here with SI constants. Tensor calculus, a matter model, and initial or boundary data are needed to solve it; quantum gravity lies beyond this description.

Quantum physics

Energy quanta, matter waves, probability amplitudes, and the limits on jointly sharp measurements.

Photon energy

E=hfE = hf

Light exchanges energy in quanta called photons. A photon’s energy depends on frequency, so ultraviolet photons carry more energy than visible or infrared photons. Increasing intensity at a fixed frequency increases photon number rather than energy per photon. OpenStax · Photons and the photoelectric effect

Photon energy: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
EEEnergy of one photonJ\mathrm{J}—
hhPlanck constantJ s\mathrm{J\,s}6.62607015×10−346.62607015\times10^{-34}
ffLight frequencyHz\mathrm{Hz}—

When it applies: Describes energy per photon at a given frequency. A light beam can contain many photons and, for broadband light, many frequencies.

De Broglie wavelength

λ=hp\lambda = \frac{h}{p}

Matter has wave properties as well as particle properties. A particle with larger momentum has a shorter wavelength. Electron diffraction reveals this behaviour, while the wavelengths of ordinary moving objects are usually too small to notice. OpenStax · De Broglie’s matter waves

De Broglie wavelength: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
λ\lambdaMatter-wave wavelengthm\mathrm{m}—
hhPlanck constantJ s\mathrm{J\,s}6.62607015×10−346.62607015\times10^{-34}
ppMagnitude of the particle’s momentumkg m s−1\mathrm{kg\,m\,s^{-1}}—

When it applies: Applies directly to a momentum component of a free particle’s state. A localised wave packet contains a range of momenta and wavelengths.

Time-dependent Schrödinger equation

iℏ∂ψ∂t=[−ℏ22m∇2+V]ψi\hbar\frac{\partial\psi}{\partial t} = \left[-\frac{\hbar^2}{2m}\nabla^2 + V\right]\psi

The wavefunction evolves according to the particle’s kinetic and potential energies. Solving this equation with suitable conditions predicts quantum states and how they change over time. It describes an amplitude whose squared magnitude determines position probabilities, rather than a classical trajectory. OpenStax · The Schrödinger equation

Time-dependent Schrödinger equation: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
ψ\psiWavefunction, depending on position and timem−3/2\mathrm{m^{-3/2}}—
iiImaginary unit11−1\sqrt{-1}
ℏ\hbarReduced Planck constantJ s\mathrm{J\,s}≈1.054571817×10−34\approx 1.054571817\times10^{-34}
mmParticle masskg\mathrm{kg}—
VVPotential energy, possibly varying with position and timeJ\mathrm{J}—
∇2\nabla^2Laplacian: sum of second spatial derivativesm−2\mathrm{m^{-2}}—
∂/∂t\partial/\partial tTime derivative at fixed positions−1\mathrm{s^{-1}}—

Wavefunction units assume normalisation over three-dimensional position space. In one or two dimensions, the normalisation gives different units.

When it applies: This is the nonrelativistic single-particle form for a scalar potential, with spin and magnetic vector potentials omitted. Relativistic particles need a different equation.

Born rule for position

P(r∈R)=∫R∣ψ(r,t)∣2 d3rP(\mathbf{r}\in\mathcal{R}) = \int_{\mathcal{R}} |\psi(\mathbf{r},t)|^2\,d^3r

The squared magnitude of the wavefunction is a position probability density. Integrating it over a region gives the probability that a position measurement finds the particle there. This connects the mathematical quantum state to observable outcomes. OpenStax · Wavefunctions and probability

Born rule for position: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
PPProbability of finding the particle in the chosen region11—
r\mathbf{r}Position vectorm\mathrm{m}—
ttTimes\mathrm{s}—
R\mathcal{R}Region of space being measured——
ψ\psiNormalised wavefunctionm−3/2\mathrm{m^{-3/2}}—
d3rd^3rVolume element in three-dimensional spacem3\mathrm{m^3}—

When it applies: For a single particle in a pure state with the wavefunction normalised over all space. The total position probability is one.

Heisenberg uncertainty principle

Δx Δpx≥ℏ2\Delta x\,\Delta p_x \geq \frac{\hbar}{2}

A quantum state cannot have both perfectly sharp position and perfectly sharp momentum along the same axis. Narrowing the position distribution broadens the range of momenta. This is a property of quantum states, not simply a limit caused by poor measuring equipment. OpenStax · Heisenberg uncertainty principle

Heisenberg uncertainty principle: symbols, definitions, SI units, and constant values
SymbolMeaningSI unitConstant value
Δx\Delta xStandard deviation of position measurements along one axism\mathrm{m}—
Δpx\Delta p_xStandard deviation of momentum measurements along that same axiskg m s−1\mathrm{kg\,m\,s^{-1}}—
ℏ\hbarReduced Planck constantJ s\mathrm{J\,s}≈1.054571817×10−34\approx 1.054571817\times10^{-34}

When it applies: The spreads refer to distributions for identically prepared states, not a classical measurement’s error bars. The inequality gives a lower bound, not a mandatory equality.