Charles-François Sturm

French-Swiss mathematician
External Websites
Also known as: Jacques-Charles-François Sturm
Quick Facts
In full:
Jacques-Charles-François Sturm
Born:
September 29, 1803, Geneva, Switzerland
Died:
December 18, 1855, Paris, France (aged 52)
Awards And Honors:
Copley Medal (1840)

Charles-François Sturm (born September 29, 1803, Geneva, Switzerland—died December 18, 1855, Paris, France) was a French mathematician whose work resulted in Sturm’s theorem, an important contribution to the theory of equations.

As tutor of the de Broglie family in Paris (1823–24), Sturm met many of the leading French scientists and mathematicians. In 1826, with the Swiss engineer Daniel Colladon, he made the first accurate determination of the velocity of sound in water, and a year later he wrote a prizewinning essay on compressible fluids.

Sturm’s theorem first appeared in Mémoire sur la résolution des équations numériques (1829; “Treatise on Numerical Equations”) and provided a complete solution to the problem—one that had been wrestled with since the time of René Descartes—of finding the number of roots (or solutions) of an algebraic equation within a given range of the variable.

Equations written on blackboard
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Published in 1834, Sturm’s work on the theory of differential equations of the second order, conducted with his friend Joseph Liouville, won him prestigious awards in France. He was elected to the French Academy of Sciences in 1836 and became a professor of mathematics at the École Polytechnique in Paris in 1838. Two years later he succeeded Siméon-Denis Poisson in the chair of mechanics at the Faculty of Sciences, Paris. Although primarily an analyst, Sturm made significant contributions to projective geometry and to the differential geometry of curves and surfaces. He also did important work on geometrical optics. Published posthumously, his Cours d’analyse de l’École Polytechnique, 2 vol. (1857–63; “Analysis Course from the École Polytechnique”), and Cours de méchanique de l’École Polytechnique, 2 vol. (1861; “Mechanics Course from the École Polytechnique”), were widely used, even in the early 20th century.

This article was most recently revised and updated by Encyclopaedia Britannica.

Sturm-Liouville problem

mathematics
Also known as: Sturm-Liouville theory, eigenvalue problem
Or:
eigenvalue problem
Key People:
Joseph Liouville
Related Topics:
boundary value
problem

Sturm-Liouville problem, in mathematics, a certain class of partial differential equations (PDEs) subject to extra constraints, known as boundary values, on the solutions. Such equations are common in both classical physics (e.g., thermal conduction) and quantum mechanics (e.g., Schrödinger equation) to describe processes where some external value (boundary value) is held constant while the system of interest transmits some form of energy.

In the mid-1830s the French mathematicians Charles-François Sturm and Joseph Liouville independently worked on the problem of heat conduction through a metal bar, in the process developing techniques for solving a large class of PDEs, the simplest of which take the form [p(x)y′]′ + [q(x) − λr(x)]y = 0 where y is some physical quantity (or the quantum mechanical wave function) and λ is a parameter, or eigenvalue, that constrains the equation so that y satisfies the boundary values at the endpoints of the interval over which the variable x ranges. If the functions p, q, and r satisfy suitable conditions, the equation will have a family of solutions, called eigenfunctions, corresponding to the eigenvalue solutions.

For the more-complicated nonhomogeneous case in which the right side of the above equation is a function, f(x), rather than zero, the eigenvalues of the corresponding homogeneous equation can be compared with the eigenvalues of the original equation. If these values are different, the problem will have a unique solution. On the other hand, if one of these eigenvalues matches, the problem will have either no solution or a whole family of solutions, depending on the properties of the function f(x).

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This article was most recently revised and updated by William L. Hosch.