# Necessary Condition for Integral Functional to have Extremum for given Function/Non-differentiable at Intermediate Point

## Theorem

Let $y, F$ be real functions.

Let $y$ be continuously differentiable for $x \in \hointr a c \cap \hointl c b$ and satisfy:

- $\map y a = A$
- $\map y b = B$

Let $J\sqbrk y$ be a functional of the form

- $\displaystyle J \sqbrk y = \int_a^b \map F {x, y, y'} \rd x$

Then the functional $J$ has a weak extremum if $y$ satisfies the following system of equations:

\(\displaystyle F_y - \dfrac \d {\d x} F_{y'}\) | \(=\) | \(\displaystyle 0\) | |||||||||||

\(\displaystyle \bigvalueat {F_{y'} } {x \mathop = c \mathop - 0}\) | \(=\) | \(\displaystyle \bigvalueat {F_{y'} } {x \mathop = c \mathop + 0}\) | |||||||||||

\(\displaystyle \bigvalueat {\paren {F - y' F_{y'} } } {x \mathop = c \mathop - 0}\) | \(=\) | \(\displaystyle \bigvalueat {\paren {F - y' F_{y'} } } {x \mathop = c \mathop + 0}\) |

where, by the use of limit from the left and limit from the right, the following abbreviations are denoted as follows:

- $\displaystyle \bigvalueat {\map y x} {x \mathop = c \mathop + 0} = \lim_{x \mathop \to c^+} \map y x$
- $\displaystyle \bigvalueat {\map y x} {x \to x \mathop = c \mathop - 0} = \lim_{x \mathop \to c^-} \map y x$

The last two equations are known as the **Weierstrass-Erdmann corner conditions**.

## Proof

Rewrite $J \sqbrk y$ as a sum of two functionals:

\(\displaystyle J \sqbrk y\) | \(=\) | \(\displaystyle \int_a^b \map F {x, y, y'} \rd x\) | |||||||||||

\(\displaystyle \) | \(=\) | \(\displaystyle \int_a^c \map F {x, y, y'} \rd x + \int_c^b \map F {x, y, y'} \rd x\) | |||||||||||

\(\displaystyle \) | \(=\) | \(\displaystyle J_1 \sqbrk y + J_2 \sqbrk y\) |

Recall that end points $x = a,x = b$ are fixed.

The function $\map y x$ has to be $C^0$ at $x = c$, but otherwise this point can move freely.

From general variation of functional, and noting that $y = \map y x$ is an extremal, write down variations for $J_1 \sqbrk y$ and $J_2 \sqbrk y$ separately:

$\displaystyle \delta J_1 = \bigvalueat {F_{y'} } {x \to c \mathop - 0} \delta y_1 + \bigvalueat {\paren {F - y' F_{y'} } } {x \to c \mathop - 0} \delta x_1$

$\displaystyle \delta J_2 = \bigvalueat {-F_{y'} } {x \to c \mathop + 0} \delta y_1 - \bigvalueat {\paren {F - y' F_{y'} } } {x \to c \mathop + 0} \delta x_1$

Note that $\delta J_1$ and $\delta J_2$ involve the same increments $\delta x_1$ and $\delta y_1$.

Since $y = \map y x$ is an extremum of $J$, we have:

\(\displaystyle \delta J\) | \(=\) | \(\displaystyle \delta J_1 + \delta J_2\) | |||||||||||

\(\displaystyle \) | \(=\) | \(\displaystyle \bigvalueat {F_{y'} } {x \mathop = c \mathop - 0} \delta y_1 + \bigvalueat {\paren {F - y' F_{y'} } } {x \mathop = c \mathop - 0} \delta x_1 - \bigvalueat {F_{y'} } {x \mathop = c \mathop + 0} \delta y_1 - \bigvalueat {\paren {F - y' F_{y'} } } {x \mathop = c \mathop + 0} \delta x_1\) | |||||||||||

\(\displaystyle \) | \(=\) | \(\displaystyle \bigvalueat {\paren{F_{y'} } {x \mathop = c \mathop - 0} - \bigvalueat {F_{y'} } {x \mathop = c \mathop + 0} } \delta y_1 + \paren {\bigvalueat {\paren {F - y' F_{y'} } } {x \mathop = c \mathop - 0} - \bigvalueat {\paren {F - y' F_{y'} } } {x \mathop = c \mathop + 0} }\) | |||||||||||

\(\displaystyle \) | \(=\) | \(\displaystyle 0\) |

Since $ \delta x_1$ and $ \delta y_1$ are arbitrary, both collections of terms have to vanish independently.

$\blacksquare$

## Sources

- 1877: G. Erdmann:
*Ueber unstetige Lösungen in der Variationsrechnung.*("On discontinuous solutions in the variational calculus.") (*J. Reine Angew. Math.***Vol. 82**: 21 – 30)

- 1963: I.M. Gelfand and S.V. Fomin:
*Calculus of Variations*... (previous) ... (next): $\S 3.15$: Broken Extremals. The Weierstrass-Erdmann Conditions