Hamilton's principle/Notation: Difference between revisions
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{{DISPLAYTITLE:Hamilton's principle — Notation}} | {{DISPLAYTITLE:Hamilton's principle — Notation}} | ||
{{Hamilton's principle map}} | |||
This page fixes the symbols used across the volume and records where they collide | This page fixes the symbols used across the volume and records where they collide | ||
with the notation of the primary sources. It exists because three collisions in | with the notation of the primary sources. It exists because three collisions in | ||
| Line 11: | Line 12: | ||
! symbol !! meaning !! introduced at | ! symbol !! meaning !! introduced at | ||
|- | |- | ||
| <math>L</math> || integrand of a functional; Lagrangian || [[Hamilton's principle/Mathematics/Functionals and the space of paths]] | | <math>L</math> || integrand of a functional; Lagrangian || [[Hamilton's principle/Mathematics/Functionals and the space of paths|Functionals and the space of paths]] | ||
|- | |- | ||
| <math>\mathcal{L}</math> || Lagrangian density, per unit volume || [[Hamilton's principle/Applications/Classical field theory]] | | <math>\mathcal{L}</math> || Lagrangian density, per unit volume || [[Hamilton's principle/Applications/Classical field theory|Classical field theory]] | ||
|- | |- | ||
| <math>J[y]</math> || a general functional || [[Hamilton's principle/Mathematics/Functionals and the space of paths]] | | <math>J[y]</math> || a general functional || [[Hamilton's principle/Mathematics/Functionals and the space of paths|Functionals and the space of paths]] | ||
|- | |- | ||
| <math>S</math> || Hamilton's action, <math>\int L\,dt</math> || [[Hamilton's principle/Mathematics/Abbreviated action: Maupertuis versus Hamilton]] | | <math>S</math> || Hamilton's action, <math>\int L\,dt</math> || [[Hamilton's principle/Mathematics/Abbreviated action: Maupertuis versus Hamilton|Abbreviated action: Maupertuis versus Hamilton]] | ||
|- | |- | ||
| <math>W</math> || abbreviated action, <math>\int \sum p\,dq</math> || [[Hamilton's principle/Mathematics/Abbreviated action: Maupertuis versus Hamilton]] | | <math>W</math> || abbreviated action, <math>\int \sum p\,dq</math> || [[Hamilton's principle/Mathematics/Abbreviated action: Maupertuis versus Hamilton|Abbreviated action: Maupertuis versus Hamilton]] | ||
|- | |- | ||
| <math>\eta</math> || a variation direction, vanishing at fixed endpoints || [[Hamilton's principle/Mathematics/The first variation]] | | <math>\eta</math> || a variation direction, vanishing at fixed endpoints || [[Hamilton's principle/Mathematics/The first variation|the first variation]] | ||
|- | |- | ||
| <math>\varepsilon</math> || the family parameter in <math>y + \varepsilon\eta</math> || [[Hamilton's principle/Mathematics/The first variation]] | | <math>\varepsilon</math> || the family parameter in <math>y + \varepsilon\eta</math> || [[Hamilton's principle/Mathematics/The first variation|the first variation]] | ||
|- | |- | ||
| <math>\delta J</math> || first variation || [[Hamilton's principle/Mathematics/The first variation]] | | <math>\delta J</math> || first variation || [[Hamilton's principle/Mathematics/The first variation|the first variation]] | ||
|- | |- | ||
| <math>\delta^2 J</math> || second variation || [[Hamilton's principle/Mathematics/The second variation]] | | <math>\delta^2 J</math> || second variation || [[Hamilton's principle/Mathematics/The second variation|the second variation]] | ||
|- | |- | ||
| <math>P</math>, <math>Q</math> || coefficients of the second variation in Legendre form || [[Hamilton's principle/Mathematics/The second variation]] | | <math>P</math>, <math>Q</math> || coefficients of the second variation in Legendre form || [[Hamilton's principle/Mathematics/The second variation|the second variation]] | ||
|- | |- | ||
| <math>p_i</math> || conjugate momentum, <math>\partial L/\partial \dot q_i</math> || [[Hamilton's principle/Mathematics/The Euler-Lagrange equation]] | | <math>p_i</math> || conjugate momentum, <math>\partial L/\partial \dot q_i</math> || [[Hamilton's principle/Mathematics/The Euler-Lagrange equation|the Euler-Lagrange equation]] | ||
|- | |- | ||
| <math>H</math> || Hamiltonian, <math>\sum p\dot q - L</math> || [[Hamilton's principle/Mathematics/The Hamiltonian and Hamilton's equations]] | | <math>H</math> || Hamiltonian, <math>\sum p\dot q - L</math> || [[Hamilton's principle/Mathematics/The Hamiltonian and Hamilton's equations|the Hamiltonian and Hamilton's equations]] | ||
|- | |- | ||
| <math>\lambda_\beta(x)</math> || multiplier '''function''', pointwise constraint || [[Hamilton's principle/Mathematics/Lagrange multipliers]] | | <math>\lambda_\beta(x)</math> || multiplier '''function''', pointwise constraint || [[Hamilton's principle/Mathematics/Lagrange multipliers|Lagrange multipliers]] | ||
|- | |- | ||
| <math>\mu_\gamma</math> || multiplier '''constant''', isoperimetric constraint || [[Hamilton's principle/Mathematics/Isoperimetric problems]] | | <math>\mu_\gamma</math> || multiplier '''constant''', isoperimetric constraint || [[Hamilton's principle/Mathematics/Isoperimetric problems|Isoperimetric problems]] | ||
|- | |- | ||
| <math>E(x,y,p,q)</math> || Weierstrass excess function || [[Hamilton's principle/Mathematics/The Weierstrass excess function]] | | <math>E(x,y,p,q)</math> || Weierstrass excess function || [[Hamilton's principle/Mathematics/The Weierstrass excess function|the Weierstrass excess function]] | ||
|- | |- | ||
| <math>\psi_i</math> || Lagrange expression, in Noether's sense || [[Hamilton's principle/Mathematics/Noether's first theorem]] | | <math>\psi_i</math> || Lagrange expression, in Noether's sense || [[Hamilton's principle/Mathematics/Noether's first theorem|Noether's first theorem]] | ||
|- | |- | ||
| <math>\Gamma^m_{ik}</math> || Christoffel symbols || [[Hamilton's principle/Applications/Geodesics]] | | <math>\Gamma^m_{ik}</math> || Christoffel symbols || [[Hamilton's principle/Applications/Geodesics|Geodesics]] | ||
|- | |- | ||
| <math>\nu</math> || Maslov index, count of conjugate points || [[Hamilton's principle/Applications/The Feynman path integral]] | | <math>\nu</math> || Maslov index, count of conjugate points || [[Hamilton's principle/Applications/The Feynman path integral|the Feynman path integral]] | ||
|} | |} | ||
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A reader who carries this volume's <math>V</math> into Hamilton's equation (A.) | A reader who carries this volume's <math>V</math> into Hamilton's equation (A.) | ||
will read it as nonsense. The quotations on | will read it as nonsense. The quotations on | ||
[[Hamilton's principle/Mathematics/Action as a function of its endpoints]] are | [[Hamilton's principle/Mathematics/Action as a function of its endpoints|Action as a function of its endpoints]] are | ||
footnoted with this warning at each occurrence. | footnoted with this warning at each occurrence. | ||
| Line 94: | Line 95: | ||
<math>S</math> and <math>W</math>, names the principles separately, and uses | <math>S</math> and <math>W</math>, names the principles separately, and uses | ||
''stationary'' rather than ''least'' for both. The distinction is the subject of | ''stationary'' rather than ''least'' for both. The distinction is the subject of | ||
[[Hamilton's principle/Mathematics/Abbreviated action: Maupertuis versus Hamilton]]. | [[Hamilton's principle/Mathematics/Abbreviated action: Maupertuis versus Hamilton|Abbreviated action: Maupertuis versus Hamilton]]. | ||
== Collision 3: <math>\delta</math> == | == Collision 3: <math>\delta</math> == | ||
| Line 113: | Line 114: | ||
The third is the trap. In Hamilton's equations (C.), (D.), (E.), (F.) and (G.), | The third is the trap. In Hamilton's equations (C.), (D.), (E.), (F.) and (G.), | ||
quoted on | quoted on | ||
[[Hamilton's principle/Mathematics/Action as a function of its endpoints]] and | [[Hamilton's principle/Mathematics/Action as a function of its endpoints|Action as a function of its endpoints]] and | ||
[[Hamilton's principle/Mathematics/The Hamilton-Jacobi equation]], every | [[Hamilton's principle/Mathematics/The Hamilton-Jacobi equation|the Hamilton-Jacobi equation]], every | ||
<math>\delta</math> in a quotient is an ordinary partial derivative. Read as | <math>\delta</math> in a quotient is an ordinary partial derivative. Read as | ||
variations they are meaningless. | variations they are meaningless. | ||
| Line 125: | Line 126: | ||
Her symbols are preserved where her equations are reproduced, on | Her symbols are preserved where her equations are reproduced, on | ||
[[Hamilton's principle/Mathematics/Noether's first theorem]], | [[Hamilton's principle/Mathematics/Noether's first theorem|Noether's first theorem]], | ||
[[Hamilton's principle/Mathematics/Noether's second theorem]] and | [[Hamilton's principle/Mathematics/Noether's second theorem|Noether's second theorem]] and | ||
[[Hamilton's principle/Mathematics/Several independent variables]]. | [[Hamilton's principle/Mathematics/Several independent variables|Several independent variables]]. | ||
{| class="wikitable" | {| class="wikitable" | ||
| Line 161: | Line 162: | ||
determinant <math>g</math> and the metric components <math>g_{ik}</math>; the | determinant <math>g</math> and the metric components <math>g_{ik}</math>; the | ||
collision is real and appears on | collision is real and appears on | ||
[[Hamilton's principle/Applications/The catenary]] and | [[Hamilton's principle/Applications/The catenary|the catenary]] and | ||
[[Hamilton's principle/Applications/The Einstein-Hilbert action]] within the same | [[Hamilton's principle/Applications/The Einstein-Hilbert action|the Einstein-Hilbert action]] within the same | ||
volume. | volume. | ||
| Line 168: | Line 169: | ||
mathematics as <math>\qquad\qquad\mathrm{(n)}</math>, because MediaWiki's TeX | mathematics as <math>\qquad\qquad\mathrm{(n)}</math>, because MediaWiki's TeX | ||
checker rejects the usual tagging command. The cross-page index is | checker rejects the usual tagging command. The cross-page index is | ||
[[Hamilton's principle/Equation index]]. | [[Hamilton's principle/Equation index|Equation index]]. | ||
== A note on <math>\vert\;\vert</math> == | == A note on <math>\vert\;\vert</math> == | ||
Latest revision as of 19:30, 15 October 2026
This page fixes the symbols used across the volume and records where they collide with the notation of the primary sources. It exists because three collisions in this subject are severe enough to make a source unreadable if they are not declared, and because a reader moving between this volume and Hamilton's essays will meet all three within a page.
Conventions of this volume
| symbol | meaning | introduced at |
|---|---|---|
| integrand of a functional; Lagrangian | Functionals and the space of paths | |
| Lagrangian density, per unit volume | Classical field theory | |
| a general functional | Functionals and the space of paths | |
| Hamilton's action, | Abbreviated action: Maupertuis versus Hamilton | |
| abbreviated action, | Abbreviated action: Maupertuis versus Hamilton | |
| a variation direction, vanishing at fixed endpoints | the first variation | |
| the family parameter in | the first variation | |
| first variation | the first variation | |
| second variation | the second variation | |
| , | coefficients of the second variation in Legendre form | the second variation |
| conjugate momentum, | the Euler-Lagrange equation | |
| Hamiltonian, | the Hamiltonian and Hamilton's equations | |
| multiplier function, pointwise constraint | Lagrange multipliers | |
| multiplier constant, isoperimetric constraint | Isoperimetric problems | |
| Weierstrass excess function | the Weierstrass excess function | |
| Lagrange expression, in Noether's sense | Noether's first theorem | |
| Christoffel symbols | Geodesics | |
| Maslov index, count of conjugate points | the Feynman path integral |
Independent variables are in the mathematics tracks and where the subject is mechanics. Greek indices run over spacetime coordinates; Latin indices over coordinates or fields.
Collision 1:
This is the collision that matters most, and it is the one that makes Hamilton's essays unreadable if it is missed.
| symbol | in this volume | in Hamilton 1834 |
|---|---|---|
| potential energy | the characteristic function, | |
| not used | the force-function, with sign opposite to potential energy | |
| kinetic energy | half the living force; same quantity |
Hamilton's is not a potential. It is the accumulated action, and his law of living force reads rather than because his is minus the potential.
A reader who carries this volume's into Hamilton's equation (A.) will read it as nonsense. The quotations on Action as a function of its endpoints are footnoted with this warning at each occurrence.
Collision 2: the action itself
| quantity | this volume | Hamilton 1834 | Hamilton 1835 | common modern usage |
|---|---|---|---|---|
| — | ||||
| or |
Hamilton's first essay works entirely with the abbreviated action. The function modern texts call the action enters only in the second essay, as a part of into which the time enters explicitly.
Both quantities are routinely called "the action" and both principles are routinely called "the principle of least action". This volume writes and , names the principles separately, and uses stationary rather than least for both. The distinction is the subject of Abbreviated action: Maupertuis versus Hamilton.
Collision 3:
carries three distinct meanings in the sources, and Hamilton uses two of them on the same page.
| usage | meaning | where |
|---|---|---|
| first variation of a functional | this volume, and Hamilton | |
| an infinitesimal change of path, this volume's | classical literature, and Hamilton | |
| partial derivative | Hamilton throughout, where a modern text writes |
The third is the trap. In Hamilton's equations (C.), (D.), (E.), (F.) and (G.), quoted on Action as a function of its endpoints and the Hamilton-Jacobi equation, every in a quotient is an ordinary partial derivative. Read as variations they are meaningless.
This volume writes for partial derivatives everywhere in its own text and preserves Hamilton's inside quotations, with a footnote at each occurrence.
Noether's notation
Her symbols are preserved where her equations are reproduced, on Noether's first theorem, Noether's second theorem and Several independent variables.
| Noether | meaning | this volume's equivalent |
|---|---|---|
| the integrand | ||
| the integral | ||
| dependent variables | fields | |
| independent variables | ||
| Lagrange expressions | left side of the Euler-Lagrange equation | |
| divergence | ||
| finite continuous group, parameters | global symmetry | |
| infinite continuous group, arbitrary functions | gauge symmetry | |
| against | total change against change at fixed argument | see her equation (9) |
The last row is not a notational nicety. The two differ by , and compressing them is where sign errors in derivations of Noether's theorem come from.
Signs and units
Metric signature, where it appears, is . Gravitational acceleration is written to avoid collision with the metric determinant and the metric components ; the collision is real and appears on the catenary and the Einstein-Hilbert action within the same volume.
Equation numbers restart at (1) on each page and are written inside the mathematics as , because MediaWiki's TeX checker rejects the usual tagging command. The cross-page index is Equation index.
A note on
Absolute values and norms are written with rather than the usual paired delimiters, throughout, for the same reason: the checker rejects the paired forms. This is a constraint of the platform, not a convention of the subject.