Jump to content

Hamilton's principle/Notation: Difference between revisions

From The Invariance Itself
hamiltons-principle>HPVBuild
Initial import of R-01
 
PMA Publisher (talk | contribs)
Published from the Principia Machina source
 
(3 intermediate revisions by one other user not shown)
Line 1: Line 1:
{{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 10: 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]]
|}
|}


Line 72: Line 74:
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 93: 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 112: 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 124: 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 160: 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 167: 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> ==
Line 175: Line 177:
paired forms. This is a constraint of the platform, not a convention of the
paired forms. This is a constraint of the platform, not a convention of the
subject.
subject.

Latest revision as of 19:30, 15 October 2026

Hamilton's principle: map
Reading the volume
How to read this volume
Notation
Glossary
Equation index
Figure gallery
Reading by level
Start here: Comparing paths
The mathematics: Functionals and the space of paths
Stationary is not least: The Jacobi condition and conjugate points
The applications: The brachistochrone
The history: Hamilton 1834 and 1835
Sources
Sources
Chronology
Related
Noether's theorems
On Physical Lines of Force

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
L integrand of a functional; Lagrangian Functionals and the space of paths
ℒ Lagrangian density, per unit volume Classical field theory
J[y] a general functional Functionals and the space of paths
S Hamilton's action, ∫Ldt Abbreviated action: Maupertuis versus Hamilton
W abbreviated action, ∫∑pdq Abbreviated action: Maupertuis versus Hamilton
η a variation direction, vanishing at fixed endpoints the first variation
ε the family parameter in y+εη the first variation
δJ first variation the first variation
δ2J second variation the second variation
P, Q coefficients of the second variation in Legendre form the second variation
pi conjugate momentum, ∂L/∂q˙i the Euler-Lagrange equation
H Hamiltonian, ∑pq˙−L the Hamiltonian and Hamilton's equations
λβ(x) multiplier function, pointwise constraint Lagrange multipliers
μγ multiplier constant, isoperimetric constraint Isoperimetric problems
E(x,y,p,q) Weierstrass excess function the Weierstrass excess function
ψi Lagrange expression, in Noether's sense Noether's first theorem
Γikm Christoffel symbols Geodesics
ν Maslov index, count of conjugate points the Feynman path integral

Independent variables are x in the mathematics tracks and t where the subject is mechanics. Greek indices run over spacetime coordinates; Latin indices over coordinates or fields.

Collision 1: V

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
V potential energy the characteristic function, ∫0t2Tdt
U not used the force-function, with sign opposite to potential energy
T kinetic energy half the living force; same quantity

Hamilton's V is not a potential. It is the accumulated action, and his law of living force reads T=U+H rather than T+V=E because his U is minus the potential.

A reader who carries this volume's V 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
∫Ldt S — S S
∫2Tdt=∫∑pdq W V V S0 or W

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 V 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 S and W, 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: δ

δ carries three distinct meanings in the sources, and Hamilton uses two of them on the same page.

usage meaning where
δJ first variation of a functional this volume, and Hamilton
δy an infinitesimal change of path, this volume's εη classical literature, and Hamilton
δV/δx partial derivative Hamilton throughout, where a modern text writes ∂V/∂x

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 δ 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 δ 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
f the integrand ℒ
I the integral S
ui dependent variables fields ϕi
xλ independent variables xα
ψi Lagrange expressions left side of the Euler-Lagrange equation
DivA divergence ∂αAα
Gρ finite continuous group, ρ parameters global symmetry
G∞ρ infinite continuous group, ρ arbitrary functions gauge symmetry
Δu against δu total change against change at fixed argument see her equation (9)

The last row is not a notational nicety. The two differ by ∑(∂u/∂xλ)Δxλ, 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 g0 to avoid collision with the metric determinant g and the metric components gik; 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 (n), 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.