Difference between revisions of "Extremal set"
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− | A collection of solutions of the [[Euler equation|Euler equation]], depending on | + | {{TEX|done}} |
+ | A collection of solutions of the [[Euler equation|Euler equation]], depending on $n$ arbitrary constants and filling without mutual intersections some part of the $(n+1)$-dimensional space. Here $n$ is the number of unknown functions $y_i(x)$, $i=1,\dots,n$, on which the functional to be minimized, | ||
− | + | $$J(y_1,\dots,y_n)=\int\limits_{x_1}^{x_2}F(x,y_1,\dots,y_n,y'_1,\dots,y'_n)dx,$$ | |
− | depends. Euler's equation is understood in the vector sense, that is, it is a system of | + | depends. Euler's equation is understood in the vector sense, that is, it is a system of $n$ ordinary differential equations of the second order: |
− | + | $$F_{y_i}-\frac d{dx}F_{y'_t}=0,\quad i=1,\dots,n.$$ | |
Two methods for constructing an extremal set are indicated below. | Two methods for constructing an extremal set are indicated below. | ||
− | Let the object of investigation be a pencil of extremals emanating from a given point | + | Let the object of investigation be a pencil of extremals emanating from a given point $M_0(x_0,y_0)$ in an $(n+1)$-dimensional space. If the extremals of the pencil do not intersect each other in some neighbourhood of $M_0$ (except at $M_0$), then they form an extremal set (a central extremal set) in this neighbourhood. |
− | Another method of constructing extremals consists in constructing the set of extremals that are transversal to a surface | + | Another method of constructing extremals consists in constructing the set of extremals that are transversal to a surface $S_0$ given in the $(n+1)$-dimensional space by an equation |
− | + | $$\phi(x,y)=0.$$ | |
If at every point of this surface the transversality conditions | If at every point of this surface the transversality conditions | ||
− | + | $$\frac{F-\sum_{i=1}^ny'_iF_{y'_i}}{\phi_x}=\frac{F_{y'_1}}{\phi_{y_1}}=\dots=\frac{F_{y'_n}}{\phi_{y_n}},$$ | |
− | + | $n$ in total, determine the value of the $n$ derivatives $y'_i$, $i=1,\dots,n$, then by taking these values as initial values of the derivatives one can draw through a point of $S_0$ an extremal that intersects $S_0$ transversally. If in a neighbourhood of this surface the above extremals do not intersect each other, then they form an extremal set (an ordinary, or proper extremal set). | |
The construction of an extremal set is the starting point in the discussion of questions connected with the construction of a field of extremals (cf. [[Extremal|Extremal]]). An extremal set is an [[Extremal field|extremal field]] if there is a one-parameter family of surfaces that intersect the extremals of the set transversally. | The construction of an extremal set is the starting point in the discussion of questions connected with the construction of a field of extremals (cf. [[Extremal|Extremal]]). An extremal set is an [[Extremal field|extremal field]] if there is a one-parameter family of surfaces that intersect the extremals of the set transversally. |
Latest revision as of 16:38, 24 November 2018
A collection of solutions of the Euler equation, depending on $n$ arbitrary constants and filling without mutual intersections some part of the $(n+1)$-dimensional space. Here $n$ is the number of unknown functions $y_i(x)$, $i=1,\dots,n$, on which the functional to be minimized,
$$J(y_1,\dots,y_n)=\int\limits_{x_1}^{x_2}F(x,y_1,\dots,y_n,y'_1,\dots,y'_n)dx,$$
depends. Euler's equation is understood in the vector sense, that is, it is a system of $n$ ordinary differential equations of the second order:
$$F_{y_i}-\frac d{dx}F_{y'_t}=0,\quad i=1,\dots,n.$$
Two methods for constructing an extremal set are indicated below.
Let the object of investigation be a pencil of extremals emanating from a given point $M_0(x_0,y_0)$ in an $(n+1)$-dimensional space. If the extremals of the pencil do not intersect each other in some neighbourhood of $M_0$ (except at $M_0$), then they form an extremal set (a central extremal set) in this neighbourhood.
Another method of constructing extremals consists in constructing the set of extremals that are transversal to a surface $S_0$ given in the $(n+1)$-dimensional space by an equation
$$\phi(x,y)=0.$$
If at every point of this surface the transversality conditions
$$\frac{F-\sum_{i=1}^ny'_iF_{y'_i}}{\phi_x}=\frac{F_{y'_1}}{\phi_{y_1}}=\dots=\frac{F_{y'_n}}{\phi_{y_n}},$$
$n$ in total, determine the value of the $n$ derivatives $y'_i$, $i=1,\dots,n$, then by taking these values as initial values of the derivatives one can draw through a point of $S_0$ an extremal that intersects $S_0$ transversally. If in a neighbourhood of this surface the above extremals do not intersect each other, then they form an extremal set (an ordinary, or proper extremal set).
The construction of an extremal set is the starting point in the discussion of questions connected with the construction of a field of extremals (cf. Extremal). An extremal set is an extremal field if there is a one-parameter family of surfaces that intersect the extremals of the set transversally.
References
[1] | V.I. Smirnov, "A course of higher mathematics" , 4 , Addison-Wesley (1964) (Translated from Russian) |
Comments
References
[a1] | I.M. Gel'fand, S.V. Fomin, "Calculus of variations" , Prentice-Hall (1963) (Translated from Russian) |
Extremal set. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Extremal_set&oldid=43478