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Lagerstrom ODEs

 

Description

Examples

Description

• 

The general form of the Lagerstrom ODE is given by the following:

> 

Lagerstrom_ode := diff(y(x),x,x)= -k*diff(y(x),x)/x-epsilon*y(x)*diff(y(x),x);

Lagerstrom_ode≔ⅆ2ⅆx2y⁡x=−k⁢ⅆⅆxy⁡xx−ε⁢y⁡x⁢ⅆⅆxy⁡x

(1)
  

See Rosenblat and Shepherd, "On the Asymptotic Solution of the Lagerstrom Model Equation".

Examples

The second order Lagerstrom ODE can be reduced to a first order ODE of Abel type once the system succeeds in finding one polynomial symmetry for it (see symgen):

> 

with⁡DEtools,odeadvisor,symgen:

> 

odeadvisor⁡Lagerstrom_ode

_Lagerstrom,_2nd_order,_with_linear_symmetries

(2)
> 

symgen⁡Lagerstrom_ode,way=3

_ξ=−x,_η=y

(3)

From which, giving the same indication directly to dsolve, you obtain the reduction of order

> 

ans≔dsolve⁡Lagerstrom_ode,way=3

ans≔y⁡x=_a⁢ⅇ∫_b⁡_aⅆ_a+c__1whereⅆⅆ_a_b⁡_a=−_a2⁢ε−_a⁢k+2⁢_a⁢_b⁡_a3+−ε⁢_a−k+3⁢_b⁡_a2,_a=x⁢y⁡x,_b⁡_a=−1x⁢y⁡x+x⁢ⅆⅆxy⁡x,x=1ⅇ∫_b⁡_aⅆ_a+c__1,y⁡x=_a⁢ⅇ∫_b⁡_aⅆ_a+c__1

(4)

For the structure of the solution above see ODESolStruc. Reductions of order can also be tested with odetest

> 

odetest⁡ans,Lagerstrom_ode

0

(5)

The reduced ODE is of Abel type and can be selected using the mouse, or as follows

> 

reduced_ode≔op⁡2,2,1,1,ans

reduced_ode≔ⅆⅆ_a_b⁡_a=−_a2⁢ε−_a⁢k+2⁢_a⁢_b⁡_a3+−ε⁢_a−k+3⁢_b⁡_a2

(6)
> 

odeadvisor⁡reduced_ode

_Abel

(7)

See Also

DEtools

odeadvisor

dsolve

quadrature

missing

reducible

linear_ODEs

exact_linear

exact_nonlinear

sym_Fx

linear_sym

Bessel

Painleve

Halm

Gegenbauer

Duffing

ellipsoidal

elliptic

erf

Emden

Jacobi

Hermite

Lagerstrom

Laguerre

Liouville

Lienard

Van_der_Pol

Titchmarsh

odeadvisor,types