DEtools
eta_k
determines the k-prolongation of the infinitesimals of a one-parameter Lie group
Calling Sequence
Parameters
Description
Examples
eta_k([xi, eta], k, y(x))
eta_k([xi, eta], k, ODE)
eta_k([xi, eta], k, y(x), ODE)
[xi, eta]
-
list of the coefficients of the symmetry generator (infinitesimals)
k
positive integer indicating the order of the required prolongation
y(x)
'dependent variable'; it can be any indeterminate function of one variable
ODE
ODE invariant under the given infinitesimals; required only if they represent dynamical symmetries
eta_k receives a pair of infinitesimals; k, the order of the required prolongation; and the dependent variable y(x), and returns the k-prolongation of eta (see infgen).
This command also works with dynamical symmetries, in which case the ODE that is assumed to be invariant under the given infinitesimals is also required as an argument. The right hand side of the given nth order ODE is then used to replace the nth order derivatives of the dependent variable appearing in the prolongation of eta.
If the infinitesimal generator of a Lie group is written as
X = (F -> xi(x,y)*diff(F,x) + eta(x,y)*diff(F,y));
X=F→ξ⁡x,y⁢∂∂x⁢F+η⁡x,y⁢∂∂y⁢F
where y(x) plays the role of the dependent variable, the k prolongation of eta is obtained as follows.
1) The linear operator A corresponding to the given ODE is built
A = (F -> diff(F,x) + _y1*diff(F,y) + _y2*diff(F,y,y) + `...` + rhs_ODE * diff(y(x),x$(n-1)));
A=F→∂∂x⁢F+_y1⁢∂∂y⁢F+_y2⁢∂2∂y2⁢F+...+rhs_ODE⁢ⅆn−1ⅆxn−1⁢y⁡x
(rhs_ODE means the right hand side of the ODE).
2) The expression
eta[n] = A(eta[n-1])- diff(y(x),x$n)*A(xi);
ηn=A⁡ηn−1−ⅆnⅆxny⁡x⁢A⁡ξ
is evaluated recursively, and in the case of dynamical symmetries, the highest order derivative is replaced by the right hand side of the ODE.
This function is part of the DEtools package, and so it can be used in the form eta_k(..) only after executing the command with(DEtools). However, it can always be accessed through the long form of the command by using DEtools[eta_k](..).
Find the infinitesimals corresponding to the one-parameter rotation group (rotations in the plane), and the first, second, and third prolongations of eta.
with⁡DEtools,eta_k,infgen
eta_k,infgen
X≔−y,x
η1=eta_k⁡X,1,y⁡x
η1=_y12+1
η2=eta_k⁡X,2,y⁡x
η2=3⁢_y2⁢_y1
η3=eta_k⁡X,3,y⁡x
η3=4⁢_y3⁢_y1+3⁢_y22
These prolongations of eta enter the expression of the extended related infinitesimal generator (a differential operator, see infgen).
infgen⁡X,3,y⁡x
_F1→−y⁢∂∂x⁢_F1+x⁢∂∂y⁢_F1+_y12+1⁢∂∂_y1⁢_F1+3⁢_y2⁢_y1⁢∂∂_y2⁢_F1+4⁢_y1⁢_y3+3⁢_y22⁢∂∂_y3⁢_F1
You can also determine point symmetries for second order ODEs. The general case is as follows:
ODE≔diff⁡y⁡x,x,x=F⁡x,y⁡x,diff⁡y⁡x,x
ODE≔ⅆ2ⅆx2y⁡x=F⁡x,y⁡x,ⅆⅆxy⁡x
X≔ξ⁡x,y,η⁡x,y
The prolongation of order 0 is just eta(x,y):
η0=eta_k⁡X,0,ODE
η0=η⁡x,y
The first and second prolongations of eta look like this:
η1=eta_k⁡X,1,ODE
η1=−∂∂yξ⁡x,y⁢_y12+∂∂yη⁡x,y−∂∂xξ⁡x,y⁢_y1+∂∂xη⁡x,y
η2=eta_k⁡X,2,ODE
η2=−∂2∂y2ξ⁡x,y⁢_y13+−2⁢∂2∂x∂yξ⁡x,y+∂2∂y2η⁡x,y⁢_y12+−3⁢F⁡x,y,_y1⁢∂∂yξ⁡x,y+2⁢∂2∂x∂yη⁡x,y−∂2∂x2ξ⁡x,y⁢_y1+F⁡x,y,_y1⁢∂∂yη⁡x,y−2⁢F⁡x,y,_y1⁢∂∂xξ⁡x,y+∂2∂x2η⁡x,y
Finally, here is the general case of a dynamical symmetry in the framework of second order ODEs and the first prolongation of eta.
X≔ξ⁡x,y,_y1,η⁡x,y,_y1
η1=−∂∂yξ⁡x,y,_y1⁢_y12+−F⁡x,y,_y1⁢∂∂_y1ξ⁡x,y,_y1+∂∂yη⁡x,y,_y1−∂∂xξ⁡x,y,_y1⁢_y1+F⁡x,y,_y1⁢∂∂_y1η⁡x,y,_y1+∂∂xη⁡x,y,_y1
See Also
dsolve/Lie
equinv
infgen
odeadvisor
PDEtools
symgen
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