TOPICS
Search

Second Variation


The second variation of a functional J at a function y measures its second-order change under an admissible perturbation h. Here y+epsilonh must remain admissible for all sufficiently small positive and negative epsilon. In the second-derivative convention, it is

 delta^2J[y;h]=(d^2)/(depsilon^2)J[y+epsilonh]|_(epsilon=0).

Some authors instead define the second variation as the coefficient of epsilon^2 in the expansion, which is half this quantity (Liberzon 2012).

For J[y]=int_a^bL(x,y,y^')dx and sufficiently smooth L,

 delta^2J[y;h]=int_a^b(L_(yy)h^2+2L_(yy^')hh^'+L_(y^'y^')(h^')^2)dx.

The subscripts denote partial derivatives, evaluated along y. For fixed endpoint values, h(a)=h(b)=0.

At an extremal, a second variation taking both positive and negative values on admissible perturbations proves that the functional has a saddle point. Nonnegativity is necessary for a local minimum, and nonpositivity is necessary for a local maximum, but either condition alone can be inconclusive. At an extremal, a sufficient condition for a strict local minimum is uniform positivity delta^2J[y;h]>=c||h||^2 for some c>0, together with an expansion whose remainder is o(||h||^2) in the same norm. The condition delta^2J[y;h]<=-c||h||^2, with the same remainder assumption, gives a strict local maximum. Pointwise positivity in each perturbation direction need not be uniform in an infinite-dimensional function space (Liberzon 2012).


See also

Calculus of Variations, First Variation, Morse Index

Explore with Wolfram|Alpha

References

Gelfand, I. M. and Fomin, S. V. Calculus of Variations. Englewood Cliffs, NJ: Prentice-Hall, 1963.Liberzon, D. Calculus of Variations and Optimal Control Theory: A Concise Introduction. Princeton, NJ: Princeton University Press, 2012. https://liberzon.csl.illinois.edu/teaching/cvoc.pdf.

Cite this as:

Weisstein, Eric W. "Second Variation." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/SecondVariation.html

Subject classifications