In classical mechanics, Maupertuis's principle (named after Pierre Louis Maupertuis) states that the path followed by a physical system is the one of least length (with a suitable interpretation of path and length). It is a special case of the more generally stated principle of least action. Using the calculus of variations, it results in an integral equation formulation of the equations of motion for the system.

Mathematical formulation

Maupertuis's principle states that the true path of a system described by ${\displaystyle N}$ generalized coordinates ${\displaystyle \mathbf {q} =\left(q_{1},q_{2},\ldots ,q_{N}\right)}$ between two specified states ${\displaystyle \mathbf {q} _{1}}$ and ${\displaystyle \mathbf {q} _{2}}$ is a minimum or a saddle point^[1] of the abbreviated action functional,

$${\displaystyle {\mathcal {S}}_{0}[\mathbf {q} (t)]\ {\stackrel {\mathrm {def} }{=}}\ \int \mathbf {p} \cdot d\mathbf {q} ,}$$

where ${\displaystyle \mathbf {p} =\left(p_{1},p_{2},\ldots ,p_{N}\right)}$ are the conjugate momenta of the generalized coordinates, defined by the equation

$${\displaystyle p_{k}\ {\stackrel {\mathrm {def} }{=}}\ {\frac {\partial L}{\partial {\dot {q}}_{k}}},}$$

where ${\displaystyle L(\mathbf {q} ,{\dot {\mathbf {q} }},t)}$ is the Lagrangian function for the system. In other words, any first-order perturbation of the path results in (at most) second-order changes in ${\displaystyle {\mathcal {S}}_{0}}$. Note that the abbreviated action ${\displaystyle {\mathcal {S}}_{0}}$ is a functional (i.e. a function from a vector space into its underlying scalar field), which in this case takes as its input a function (i.e. the paths between the two specified states).

Jacobi's formulation

For many systems, the kinetic energy ${\displaystyle T}$ is quadratic in the generalized velocities ${\displaystyle {\dot {\mathbf {q} }}}$

$${\displaystyle T={\frac {1}{2}}{\dot {\mathbf {q} }}\ \mathbf {M} \ {\dot {\mathbf {q} }}^{\intercal }}$$

although the mass tensor ${\displaystyle \mathbf {M} }$ may be a complicated function of the generalized coordinates ${\displaystyle \mathbf {q} }$. For such systems, a simple relation relates the kinetic energy, the generalized momenta and the generalized velocities

$${\displaystyle 2T=\mathbf {p} \cdot {\dot {\mathbf {q} }}}$$

provided that the potential energy ${\displaystyle V(\mathbf {q} )}$ does not involve the generalized velocities. By defining a normalized distance or metric ${\displaystyle ds}$ in the space of generalized coordinates

$${\displaystyle ds^{2}=d\mathbf {q} \ \mathbf {M} \ d\mathbf {q^{\intercal }} }$$

one may immediately recognize the mass tensor as a metric tensor. The kinetic energy may be written in a massless form

$${\displaystyle T={\frac {1}{2}}\left({\frac {ds}{dt}}\right)^{2}}$$

or,

$${\displaystyle 2Tdt={\sqrt {2T}}\ ds.}$$

Therefore, the abbreviated action can be written

$${\displaystyle {\mathcal {S}}_{0}\ {\stackrel {\mathrm {def} }{=}}\ \int \mathbf {p} \cdot d\mathbf {q} =\int ds\,{\sqrt {2}}{\sqrt {E_{\text{tot}}-V(\mathbf {q} )}}}$$

since the kinetic energy ${\displaystyle T=E_{\text{tot}}-V(\mathbf {q} )}$ equals the (constant) total energy ${\displaystyle E_{\text{tot}}}$ minus the potential energy ${\displaystyle V(\mathbf {q} )}$. In particular, if the potential energy is a constant, then Jacobi's principle reduces to minimizing the path length ${\textstyle s=\int ds}$ in the space of the generalized coordinates, which is equivalent to Hertz's principle of least curvature.

Comparison with Hamilton's principle

Hamilton's principle and Maupertuis's principle are occasionally confused with each other and both have been called the principle of least action. They differ from each other in three important ways:

• their definition of the action...
  Hamilton's principle uses ${\displaystyle {\mathcal {S}}\ {\stackrel {\mathrm {def} }{=}}\ \int L\,dt}$, the integral of the Lagrangian over time, varied between two fixed end times ${\displaystyle t_{1}}$, ${\displaystyle t_{2}}$ and endpoints ${\displaystyle q_{1}}$, ${\displaystyle q_{2}}$. By contrast, Maupertuis's principle uses the abbreviated action integral over the generalized coordinates, varied along all constant energy paths ending at ${\displaystyle \mathbf {q} _{1}}$ and ${\displaystyle \mathbf {q} _{2}}$.
• the solution that they determine...
  Hamilton's principle determines the trajectory ${\displaystyle \mathbf {q} (t)}$ as a function of time, whereas Maupertuis's principle determines only the shape of the trajectory in the generalized coordinates. For example, Maupertuis's principle determines the shape of the ellipse on which a particle moves under the influence of an inverse-square central force such as gravity, but does not describe per se how the particle moves along that trajectory. (However, this time parameterization may be determined from the trajectory itself in subsequent calculations using the conservation of energy.) By contrast, Hamilton's principle directly specifies the motion along the ellipse as a function of time.
• ...and the constraints on the variation.
  Maupertuis's principle requires that the two endpoint states ${\displaystyle q_{1}}$ and ${\displaystyle q_{2}}$ be given and that energy be conserved along every trajectory. By contrast, Hamilton's principle does not require the conservation of energy, but does require that the endpoint times ${\displaystyle t_{1}}$ and ${\displaystyle t_{2}}$ be specified as well as the endpoint states ${\displaystyle q_{1}}$ and ${\displaystyle q_{2}}$.

History

Maupertuis was the first to publish a principle of least action, as a way of adapting Fermat's principle for waves to a corpuscular (particle) theory of light.^[2]: 96 Pierre de Fermat had explained Snell's law for the refraction of light by assuming light follows the path of shortest time, not distance. This troubled Maupertuis, since he felt that time and distance should be on an equal footing: "why should light prefer the path of shortest time over that of distance?" Maupertuis defined his action as ${\textstyle \int v\,ds}$, which was to be minimized over all paths connecting two specified points. Here ${\displaystyle v}$ is the velocity of light the corpuscular theory. Fermat had minimized ${\textstyle \int \,ds/v}$ where ${\displaystyle v}$ is wave velocity; the two velocities are reciprocal so the two forms are equivalent.

See also

• Analytical mechanics
• Hamilton's principle
• Gauss's principle of least constraint (also describes Hertz's principle of least curvature)
• Hamilton–Jacobi equation

References

• Pierre Louis Maupertuis, Accord de différentes loix de la nature qui avoient jusqu'ici paru incompatibles (original 1744 French text); Accord between different laws of Nature that seemed incompatible (English translation)
• Leonhard Euler, Methodus inveniendi/Additamentum II (original 1744 Latin text); Methodus inveniendi/Appendix 2 (English translation)
• Pierre Louis Maupertuis, Les loix du mouvement et du repos déduites d'un principe metaphysique (original 1746 French text); Derivation of the laws of motion and equilibrium from a metaphysical principle (English translation)
• Leonhard Euler, Exposé concernant l'examen de la lettre de M. de Leibnitz (original 1752 French text); Investigation of the letter of Leibniz (English translation)
• König J. S. "De universali principio aequilibrii et motus", Nova Acta Eruditorum, 1751, 125–135, 162–176.
• J. J. O'Connor and E. F. Robertson, "The Berlin Academy and forgery", (2003), at The MacTutor History of Mathematics archive.
• C. I. Gerhardt, (1898) "Über die vier Briefe von Leibniz, die Samuel König in dem Appel au public, Leide MDCCLIII, veröffentlicht hat", Sitzungsberichte der Königlich Preussischen Akademie der Wissenschaften, I, 419–427.
• W. Kabitz, (1913) "Über eine in Gotha aufgefundene Abschrift des von S. König in seinem Streite mit Maupertuis und der Akademie veröffentlichten, seinerzeit für unecht erklärten Leibnizbriefes", Sitzungsberichte der Königlich Preussischen Akademie der Wissenschaften, II, 632–638.
• L. D. Landau and E. M. Lifshitz, (1976) Mechanics, 3rd. ed., Pergamon Press, pp. 140–143. ISBN 0-08-021022-8 (hardcover) and ISBN 0-08-029141-4 (softcover)
• G. C. J. Jacobi, Vorlesungen über Dynamik, gehalten an der Universität Königsberg im Wintersemester 1842–1843. A. Clebsch (ed.) (1866); Reimer; Berlin. 290 pages, available online Œuvres complètes volume 8 at Gallica-Math from the Gallica Bibliothèque nationale de France.
• H. Hertz, (1896) Principles of Mechanics, in Miscellaneous Papers, vol. III, Macmillan.
• V.V. Rumyantsev (2001) [1994], "Hertz's principle of least curvature", Encyclopedia of Mathematics, EMS Press