Beltrami identity

Beltrami identity

The Beltrami identity is an identity in the calculus of variations. It says that a function "u" which is an extremal of the integral

:I(u)=int_a^b f(x,u,u') , dx

satisfies the differential equation

:frac{d}{dx}left(f-u'frac{partial f}{partial u'} ight)-frac{partial f}{partial x}=0.

Proof

The Euler-Lagrange equation tells that

:frac{partial f}{partial u}-frac{d}{dx}frac{partial f}{partial u'}=0.

Now consider the total differential of functional f(x,u,u'). Substituting the Euler-Lagrange equation into it, we have

:egin{align}frac{df}{dx} &= frac{partial f}{partial x} + frac{partial f}{partial u} u' + frac{partial f}{partial u'} u" \& = frac{partial f}{partial x} + left(frac{d}{dx}frac{partial f}{partial u'} ight) u' + frac{partial f}{partial u'} u".end{align}

Therefore,

:frac{d}{dx}left(f-u'frac{partial f}{partial u'} ight)-frac{partial f}{partial x}=0.

Application

In case the functional "f" is independent of "x", then the Beltrami identity can be simplified into

:egin{align}frac{d}{dx}left(f-u'frac{partial f}{partial u'} ight) &=0 \f-u'frac{partial f}{partial u'} &= ext{constant} \end{align}

Using the above form is an easier approach to solve for the optimal function "u" than directly applying the Euler-Lagrange equation.


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