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Beltrami identity

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The Beltrami identity, named after Eugenio Beltrami, is a simplified and less general version of the Euler–Lagrange equation in the calculus of variations.

Contents

The Euler–Lagrange equation serves to extremize action functionals of the form

I [ u ] = a b L [ x , u ( x ) , u ( x ) ] d x ,

where a, b are constants and u′(x) = du / dx.

For the special case of L / ∂x = 0, the Euler–Lagrange equation reduces to the Beltrami identity,

where C is a constant.

Derivation

The following derivation of the Beltrami identity starts with the Euler–Lagrange equation,

L u = d d x L u .

Multiplying both sides by u,

u L u = u d d x L u .

According to the chain rule,

d L d x = L u u + L u u + L x ,

where u′′ = du′/dx = d2u / dx2.

Rearranging this yields

u L u = d L d x L u u L x .

Thus, substituting this expression for u′ ∂L/∂u into the second equation of this derivation,

d L d x L u u L x u d d x L u = 0 .

By the product rule, the last term is re-expressed as

u d d x L u = d d x ( L u u ) L u u ,

and rearranging,

d d x ( L u L u ) = L x .

For the case of L / ∂x = 0, this reduces to

d d x ( L u L u ) = 0 ,

so that taking the antiderivative results in the Beltrami identity,

L u L u = C ,

where C is a constant.

Application

An example of an application of the Beltrami identity is the Brachistochrone problem, which involves finding the curve y = y(x) that minimizes the integral

I [ y ] = 0 a 1 + y 2 y d x .

The integrand

L ( y , y ) = 1 + y 2 y

does not depend explicitly on the variable of integration x, so the Beltrami identity applies,

L y L y = C .

Substituting for L and simplifying,

y ( 1 + y 2 ) = 1 / C 2     (constant) ,

which can be solved with the result put in the form of parametric equations

x = A ( ϕ sin ϕ ) y = A ( 1 cos ϕ )

with A being half the above constant, 1/(2C ²), and φ being a variable. These are the parametric equations for a cycloid.

References

Beltrami identity Wikipedia


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