method

Hamiltonian mechanics

Hamiltonian mechanics is a reformulation of classical mechanics that describes the evolution of a system using generalized coordinates and momenta.
28 related articles · 5 formulas · 1 who worked here

Description

The protagonist of Hamiltonian mechanics is the Hamiltonian function, i.e., the total energy of the system expressed in terms of coordinates and momenta. Unlike the Newtonian approach, where force causes acceleration, here energy reigns. A pair of Hamilton's equations (the first linking velocity to momentum, the second linking change in momentum to force) turns mechanics into the geometry of phase space: each state is a point, and evolution is a line on the energy landscape. This perspective clarifies why energy, momentum, and other quantities are conserved.

History

The idea grew out of geometric optics. William Rowan Hamilton in 1833 applied the optical-mechanical analogy to rewrite Newton's laws in terms of energy. Later, Henri Poincaré used Hamiltonian methods to analyze the stability of the Solar System, laying the foundation for chaos theory. Emmy Noether proved that every continuous symmetry of a Hamiltonian system corresponds to a conserved quantity — a result that cemented the foundation of all modern physics.

How it works

The Hamiltonian function H generates a vector field in phase space. The integral curves of this field are the system's trajectories. If H does not depend explicitly on time, energy is conserved. In the quantum picture, the Hamiltonian becomes an operator that determines the evolution of the wave function via the Schrödinger equation. Canonical transformations here become unitary transformations, and Liouville's theorem becomes the unitarity of quantum evolution.

In practice

Calculating satellite orbits, modeling quantum computers, synthesizing new materials with desired properties.

Fun fact

The formalism turned out to be so elegant that it crossed over into quantum mechanics almost unchanged: the Hamiltonian operator became the main tool for describing particles and fields.

Concept graph →

Formulas

$$H = -\sum_{\langle i,j \rangle} J_{ij} \mathbf{S}_i \cdot \mathbf{S}_j$$
Describes the energy of interacting spins with exchange coupling.
What is in the formula
HvariableHamiltonian (total energy operator) — hamiltonian joule
J_{ij}variableExchange coupling constant between sites i and j — exchange coupling joule
\mathbf{S}_ivariableSpin operator at site i — spin operator
\mathbf{S}_jvariableSpin operator at site j — spin operator
\sum_{\langle i,j \roperatorSummation over all pairs of adjacent lattice sites — sum over nearest neighbors
h=\sum_nj_n{s}_n*{s}_{n+1} · 2606.29281
$$H_{ ext{eff}} = H_0 + rac{[H_{-1}, H_{+1}]}{ ext{frequency}}$$
Approximates the static Hamiltonian under high-frequency driving.
What is in the formula
H_effvariableeffective static Hamiltonian — hamiltonian joule
H_0variabletime-averaged Hamiltonian — hamiltonian joule
H_{-1}variablefirst negative Fourier component of the Hamiltonian — hamiltonian joule
H_{+1}variablefirst positive Fourier component of the Hamiltonian — hamiltonian joule
frequencyvariabledriving frequency — angular frequency radian per second
[ , ]operatormeasures the non-commutativity of two operators — commutator
h_{{eff}}\approxh_0+\frac{[h_{-1},h_{+1}]}{ħω} · 2606.31867
$$H = -it \sum_j \gamma_{2j} \gamma_{2j+1}$$
Hamiltonian for a Kitaev chain with Majorana fermion pairing.
What is in the formula
HvariableHamiltonian operator — hamiltonian joule
tvariablehopping amplitude — energy joule
γ_{2j}variableMajorana operator at site 2j — majorana operator
γ_{2j+1}variableMajorana operator at site 2j+1 — majorana operator
∑operatorsum over lattice sites j — summation
h=-it\sum_{j=1}^{l-1}γ_{2j}γ_{2j+1} · 2606.25653
$$\ddot{x} + \gamma \dot{x} + \omega^2 x = \eta(t)$$
Describes motion with damping, restoring force, and random driving.
What is in the formula
xvariablePosition of the particle — position metre
γvariableDamping coefficient — damping coefficient per second
ωvariableNatural angular frequency of the oscillator — angular frequency radian per second
η(t)variableRandom force (noise) as a function of time — random force newton per kilogram
d²/dt²operatorSecond derivative with respect to time — second time derivative
d/dtoperatorFirst derivative with respect to time — first time derivative
\ddot{h}+γ\dot{h}+ω^2h=\eta(t) · 2607.28209v1
$$\hat{H}_{\text{ex}} = J (\hat{\sigma}_+ \hat{\sigma}_- + \hat{\sigma}_- \hat{\sigma}_+)$$
Exchange interaction couples spin raising and lowering operators.
What is in the formula
Jvariableexchange coupling constant — exchange coupling constant joule
σ₊variablespin raising operator — spin raising operator
σ₋variablespin lowering operator — spin lowering operator
\hat{h}_{{eff}}=\lambda_{{nt}}(\hat{σ}_{+}\hat{σ}_{t}^{-}+\hat{σ}_{t}^{+}\hat{σ}_{-}) · 2505.00266v1

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