Difference between revisions of "Differential equation with total differential"
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An ordinary differential equation | An ordinary differential equation | ||
− | + | $$ \tag{1 } | |
+ | F ( x , y , y ^ \prime \dots y ^ {( n) } ) = 0 | ||
+ | $$ | ||
whose left-hand side is a total derivative: | whose left-hand side is a total derivative: | ||
− | + | $$ | |
+ | |||
+ | \frac{d}{dx} | ||
+ | \Phi ( x , y , y ^ \prime \dots y ^ {( n - 1 ) } | ||
+ | ) = 0 . | ||
+ | $$ | ||
− | In other words, equation (1) is a differential equation with total differential if there exists a differentiable function | + | In other words, equation (1) is a differential equation with total differential if there exists a differentiable function $ \Phi ( x , u _ {0} \dots u _ {n - 1 } ) $ |
+ | such that | ||
− | + | $$ | |
+ | F ( x , u _ {0} \dots u _ {n} ) \equiv \Phi _ {x} ^ \prime | ||
+ | + u _ {1} \Phi _ {u _ {0} } ^ \prime + | ||
+ | + \dots + u _ {n} \Phi _ {u _ {n-} 1 } ^ \prime | ||
+ | $$ | ||
− | identically with respect to all arguments. The solution of a differential equation with total differential of order | + | identically with respect to all arguments. The solution of a differential equation with total differential of order $ n $ |
+ | is reduced to solving an equation of order $ ( n - 1 ) $: | ||
− | + | $$ | |
+ | \Phi ( x , y , y ^ \prime \dots y ^ {( n - 1 ) } ) = C ,\ \ | ||
+ | C = \textrm{ const } . | ||
+ | $$ | ||
− | Let | + | Let $ F ( x, u _ {0} \dots u _ {n} ) $ |
+ | be an $ n $ | ||
+ | times continuously-differentiable function and let $ \Phi ( x , u _ {0} \dots u _ {n - 1 } ) $ | ||
+ | be a function having continuous partial derivatives up to and including the second order. Let | ||
− | + | $$ | |
+ | \Delta \Phi = \Phi _ {x} ^ \prime + u _ {1} \Phi _ {u _ {0} } ^ \prime | ||
+ | + \dots + u _ {n} \Phi _ {u _ {n-} 1 } ^ \prime , | ||
+ | $$ | ||
− | + | $$ | |
+ | \Delta _ {0} F = F _ {u _ {n} } ^ { \prime } ,\ \Delta _ \nu F = F _ {u _ {n - \nu } } ^ { \prime } - \Delta ( | ||
+ | \Delta _ {\nu - 1 } F ) ,\ \nu = 1 \dots n . | ||
+ | $$ | ||
− | For equation (1) to be a differential equation with total differential it is sufficient that the functions | + | For equation (1) to be a differential equation with total differential it is sufficient that the functions $ \Delta _ \nu F $, |
+ | $ \nu = 0 \dots n $, | ||
+ | are independent of $ u _ {n} $ | ||
+ | and that $ \Delta _ {n } F = 0 $[[#References|[1]]]. In particular, $ u _ {n} $ | ||
+ | may enter $ F $ | ||
+ | in a linear manner only. | ||
The first-order equation | The first-order equation | ||
− | + | $$ \tag{2 } | |
+ | M ( x , y ) + N ( x , y ) y ^ \prime = 0 , | ||
+ | $$ | ||
− | where the functions | + | where the functions $ M $, |
+ | $ N $, | ||
+ | $ M _ {y} ^ { \prime } $, | ||
+ | and $ N _ {x} ^ { \prime } $ | ||
+ | are defined and continuous in an open simply-connected domain $ D $ | ||
+ | of the $ ( x , y ) $- | ||
+ | plane and $ M ^ {2} + N ^ {2} > 0 $ | ||
+ | in $ D $, | ||
+ | is a differential equation with total differential if and only if | ||
− | + | $$ | |
+ | M _ {y} ^ { \prime } ( x , y ) \equiv N _ {x} ^ { \prime } | ||
+ | ( x , y ) \ \mathop{\rm in} D . | ||
+ | $$ | ||
− | The general solution of equation (2) with total differential has the form | + | The general solution of equation (2) with total differential has the form $ \Phi ( x , y ) = 0 $, |
+ | where | ||
− | + | $$ | |
+ | \Phi ( x , y ) = \int\limits _ {( x _ {0} , y _ {0} ) } ^ { {( } x , y ) } M ( x , y ) dx + N ( x , y ) dy , | ||
+ | $$ | ||
− | and the integral is taken over any rectifiable curve lying inside | + | and the integral is taken over any rectifiable curve lying inside $ D $ |
+ | and joining an arbitrary fixed point $ ( x _ {0} , y _ {0} ) \in D $ | ||
+ | with the point $ ( x , y ) $[[#References|[2]]]. Equation (2) (in the general case, an equation (1) which is linear with respect to $ y ^ {(} n) $) | ||
+ | can, under certain conditions, be reduced to a differential equation with total differential by multiplying by an [[Integrating factor|integrating factor]]. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> E. Kamke, "Differentialgleichungen: Lösungen und Lösungsmethoden" , '''1. Gewöhnliche Differentialgleichungen''' , Chelsea, reprint (1947)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> N.P. Erugin, "A general course in differential equations" , Minsk (1972) (In Russian)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> E. Kamke, "Differentialgleichungen: Lösungen und Lösungsmethoden" , '''1. Gewöhnliche Differentialgleichungen''' , Chelsea, reprint (1947)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> N.P. Erugin, "A general course in differential equations" , Minsk (1972) (In Russian)</TD></TR></table> |
Latest revision as of 17:33, 5 June 2020
An ordinary differential equation
$$ \tag{1 } F ( x , y , y ^ \prime \dots y ^ {( n) } ) = 0 $$
whose left-hand side is a total derivative:
$$ \frac{d}{dx} \Phi ( x , y , y ^ \prime \dots y ^ {( n - 1 ) } ) = 0 . $$
In other words, equation (1) is a differential equation with total differential if there exists a differentiable function $ \Phi ( x , u _ {0} \dots u _ {n - 1 } ) $ such that
$$ F ( x , u _ {0} \dots u _ {n} ) \equiv \Phi _ {x} ^ \prime + u _ {1} \Phi _ {u _ {0} } ^ \prime + + \dots + u _ {n} \Phi _ {u _ {n-} 1 } ^ \prime $$
identically with respect to all arguments. The solution of a differential equation with total differential of order $ n $ is reduced to solving an equation of order $ ( n - 1 ) $:
$$ \Phi ( x , y , y ^ \prime \dots y ^ {( n - 1 ) } ) = C ,\ \ C = \textrm{ const } . $$
Let $ F ( x, u _ {0} \dots u _ {n} ) $ be an $ n $ times continuously-differentiable function and let $ \Phi ( x , u _ {0} \dots u _ {n - 1 } ) $ be a function having continuous partial derivatives up to and including the second order. Let
$$ \Delta \Phi = \Phi _ {x} ^ \prime + u _ {1} \Phi _ {u _ {0} } ^ \prime + \dots + u _ {n} \Phi _ {u _ {n-} 1 } ^ \prime , $$
$$ \Delta _ {0} F = F _ {u _ {n} } ^ { \prime } ,\ \Delta _ \nu F = F _ {u _ {n - \nu } } ^ { \prime } - \Delta ( \Delta _ {\nu - 1 } F ) ,\ \nu = 1 \dots n . $$
For equation (1) to be a differential equation with total differential it is sufficient that the functions $ \Delta _ \nu F $, $ \nu = 0 \dots n $, are independent of $ u _ {n} $ and that $ \Delta _ {n } F = 0 $[1]. In particular, $ u _ {n} $ may enter $ F $ in a linear manner only.
The first-order equation
$$ \tag{2 } M ( x , y ) + N ( x , y ) y ^ \prime = 0 , $$
where the functions $ M $, $ N $, $ M _ {y} ^ { \prime } $, and $ N _ {x} ^ { \prime } $ are defined and continuous in an open simply-connected domain $ D $ of the $ ( x , y ) $- plane and $ M ^ {2} + N ^ {2} > 0 $ in $ D $, is a differential equation with total differential if and only if
$$ M _ {y} ^ { \prime } ( x , y ) \equiv N _ {x} ^ { \prime } ( x , y ) \ \mathop{\rm in} D . $$
The general solution of equation (2) with total differential has the form $ \Phi ( x , y ) = 0 $, where
$$ \Phi ( x , y ) = \int\limits _ {( x _ {0} , y _ {0} ) } ^ { {( } x , y ) } M ( x , y ) dx + N ( x , y ) dy , $$
and the integral is taken over any rectifiable curve lying inside $ D $ and joining an arbitrary fixed point $ ( x _ {0} , y _ {0} ) \in D $ with the point $ ( x , y ) $[2]. Equation (2) (in the general case, an equation (1) which is linear with respect to $ y ^ {(} n) $) can, under certain conditions, be reduced to a differential equation with total differential by multiplying by an integrating factor.
References
[1] | E. Kamke, "Differentialgleichungen: Lösungen und Lösungsmethoden" , 1. Gewöhnliche Differentialgleichungen , Chelsea, reprint (1947) |
[2] | N.P. Erugin, "A general course in differential equations" , Minsk (1972) (In Russian) |
Differential equation with total differential. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Differential_equation_with_total_differential&oldid=46680