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Introduction to Symmetry Analysis. Chapter 8 - Ordinary Differential Equations. Brian Cantwell Department of Aeronautics and Astronautics Stanford University. 8.1 Extension of Lie Groups in the Plane. The Extended Transformation is a Group. Two transformations of the extended group.
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Introduction to Symmetry Analysis Chapter 8 - Ordinary Differential Equations Brian Cantwell Department of Aeronautics and Astronautics Stanford University
The Extended Transformation is a Group Two transformations of the extended group Compose the two transformations
The last relation is rearranged to read Differentiating F and G gives Comparing the expressions in parentheses we have The composed transformation is in exactly the same form as the original transformation!
Finite transformation of the second derivative The twice extended finite transformation is
Infinitesimal transformation of the second derivative Recall the infinitesimal transformation of coordinates where Substitute Expand and retain only the lowest order terms
The once-extended infinitesimal transformation in the plane is where the infinitesimal function fully written out is
The twice-extended infinitesimal transformation in the plane is Expand and retain only the lowest order terms where
The infinitesimal function transforming third derivatives is
The infinitesimal transformation of higher order derivatives Expand and retain only the lowest order terms. The p times extended infinitesimal transformation is where
8.2 Expansion of an ODE in a Lie Series - the Invariance Condition for ODEs
The characteristic equations associated with extended groups are
The general second-order ordinary differential equation is invariant under the twice-extended group if and only if
Consider the case of the simplest second-order ODE The invariance condition is Fully written out the invariance condition is For invariance this equation must be satisfied subject to the condition that y is a solution of
The determining equations of the group are These equations can be used to work out the unknown infinitesimals.
Assume that the infinitesimals can be written as a multivariate power series Insert these series into the determining equations
The coefficients must satisfy the following algebraic system Finally the infinitesimals are
The two parameter group of the Blasius equation The invariance condition
Now gather coefficients of like products of derivatives of y
The function y[x] is a solution of the Blasius equation. This is a constraint on the invariance condition that can be used to eliminate the third derivative.
Further simplify and
Finally the determining equations are From which the two parameter group of the Blasius equation is determined to be