Solution to Nonlinear System of Differential EquationsSolution of system of linearly dependent equations.Solve numerical system of nonlinear equations?Finding a Lyapunov function for the differential system $x_1'=-8x_1^3-x_2$, $x_2'=-4x_2-4x_1^3$Solving a system of partial differential equations consist of 6 equations on 9 variables by using MatlabBendixson's condition for existence of limit cycle for a nonlinear systemNumerically solving a system of linear 2nd order differential equationsNonlinear equations systemsOrdinary Differential Equation with 3 unknownsTrouble with numerically solving this system of nonlinear ODEsHelp solving a system of differential equations
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Solution to Nonlinear System of Differential Equations
Solution of system of linearly dependent equations.Solve numerical system of nonlinear equations?Finding a Lyapunov function for the differential system $x_1'=-8x_1^3-x_2$, $x_2'=-4x_2-4x_1^3$Solving a system of partial differential equations consist of 6 equations on 9 variables by using MatlabBendixson's condition for existence of limit cycle for a nonlinear systemNumerically solving a system of linear 2nd order differential equationsNonlinear equations systemsOrdinary Differential Equation with 3 unknownsTrouble with numerically solving this system of nonlinear ODEsHelp solving a system of differential equations
$begingroup$
I am working on a optimal control problem, specifically the design of a hypersonic aircraft nose. When minimizing the drag coefficient, I am led to the following system of differential equations:
$$
x_1' = -x_2
$$
$$
x_3' = frac-4x_2^31+x_2^2
$$
$$
x_3 = frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
$$
with the boundary/initial conditions
$$
x_1(0) = a, qquad 4x_1(l) = x_3(l),
$$
where $l$ is just the endpoint, i.e. $xin[0,l]$. Is it possible to solve this system analytically, or will I have to resort to a numerical solution?
If it helps, the source of these equations comes from the Hamiltonian
$$
H(r,u,p) = frac4ru^31+u^2-pu,
$$
with the necessary conditions
$$
fracpartial Hpartial u = 0, qquad p' = fracdpdx = -fracpartial Hpartial r
$$
I just relabeled the variables as $x_1 equiv r, x_2 equiv u, x_3 equiv p$.
ordinary-differential-equations nonlinear-system optimal-control nonlinear-analysis
$endgroup$
add a comment |
$begingroup$
I am working on a optimal control problem, specifically the design of a hypersonic aircraft nose. When minimizing the drag coefficient, I am led to the following system of differential equations:
$$
x_1' = -x_2
$$
$$
x_3' = frac-4x_2^31+x_2^2
$$
$$
x_3 = frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
$$
with the boundary/initial conditions
$$
x_1(0) = a, qquad 4x_1(l) = x_3(l),
$$
where $l$ is just the endpoint, i.e. $xin[0,l]$. Is it possible to solve this system analytically, or will I have to resort to a numerical solution?
If it helps, the source of these equations comes from the Hamiltonian
$$
H(r,u,p) = frac4ru^31+u^2-pu,
$$
with the necessary conditions
$$
fracpartial Hpartial u = 0, qquad p' = fracdpdx = -fracpartial Hpartial r
$$
I just relabeled the variables as $x_1 equiv r, x_2 equiv u, x_3 equiv p$.
ordinary-differential-equations nonlinear-system optimal-control nonlinear-analysis
$endgroup$
2
$begingroup$
Is there (supposed to be) an equation for $x_2'$? Or, how does $x_2$ evolve? Cheers!
$endgroup$
– Robert Lewis
Mar 30 at 2:29
1
$begingroup$
No equation for $x_2'$ unfortunately. $x_2 = u(x)$ would be the control input for this system, and the necessary conditions give this system of equations.
$endgroup$
– Josh Pilipovsky
Mar 30 at 2:33
add a comment |
$begingroup$
I am working on a optimal control problem, specifically the design of a hypersonic aircraft nose. When minimizing the drag coefficient, I am led to the following system of differential equations:
$$
x_1' = -x_2
$$
$$
x_3' = frac-4x_2^31+x_2^2
$$
$$
x_3 = frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
$$
with the boundary/initial conditions
$$
x_1(0) = a, qquad 4x_1(l) = x_3(l),
$$
where $l$ is just the endpoint, i.e. $xin[0,l]$. Is it possible to solve this system analytically, or will I have to resort to a numerical solution?
If it helps, the source of these equations comes from the Hamiltonian
$$
H(r,u,p) = frac4ru^31+u^2-pu,
$$
with the necessary conditions
$$
fracpartial Hpartial u = 0, qquad p' = fracdpdx = -fracpartial Hpartial r
$$
I just relabeled the variables as $x_1 equiv r, x_2 equiv u, x_3 equiv p$.
ordinary-differential-equations nonlinear-system optimal-control nonlinear-analysis
$endgroup$
I am working on a optimal control problem, specifically the design of a hypersonic aircraft nose. When minimizing the drag coefficient, I am led to the following system of differential equations:
$$
x_1' = -x_2
$$
$$
x_3' = frac-4x_2^31+x_2^2
$$
$$
x_3 = frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
$$
with the boundary/initial conditions
$$
x_1(0) = a, qquad 4x_1(l) = x_3(l),
$$
where $l$ is just the endpoint, i.e. $xin[0,l]$. Is it possible to solve this system analytically, or will I have to resort to a numerical solution?
If it helps, the source of these equations comes from the Hamiltonian
$$
H(r,u,p) = frac4ru^31+u^2-pu,
$$
with the necessary conditions
$$
fracpartial Hpartial u = 0, qquad p' = fracdpdx = -fracpartial Hpartial r
$$
I just relabeled the variables as $x_1 equiv r, x_2 equiv u, x_3 equiv p$.
ordinary-differential-equations nonlinear-system optimal-control nonlinear-analysis
ordinary-differential-equations nonlinear-system optimal-control nonlinear-analysis
edited Mar 30 at 2:40
Josh Pilipovsky
asked Mar 30 at 2:22
Josh PilipovskyJosh Pilipovsky
1033
1033
2
$begingroup$
Is there (supposed to be) an equation for $x_2'$? Or, how does $x_2$ evolve? Cheers!
$endgroup$
– Robert Lewis
Mar 30 at 2:29
1
$begingroup$
No equation for $x_2'$ unfortunately. $x_2 = u(x)$ would be the control input for this system, and the necessary conditions give this system of equations.
$endgroup$
– Josh Pilipovsky
Mar 30 at 2:33
add a comment |
2
$begingroup$
Is there (supposed to be) an equation for $x_2'$? Or, how does $x_2$ evolve? Cheers!
$endgroup$
– Robert Lewis
Mar 30 at 2:29
1
$begingroup$
No equation for $x_2'$ unfortunately. $x_2 = u(x)$ would be the control input for this system, and the necessary conditions give this system of equations.
$endgroup$
– Josh Pilipovsky
Mar 30 at 2:33
2
2
$begingroup$
Is there (supposed to be) an equation for $x_2'$? Or, how does $x_2$ evolve? Cheers!
$endgroup$
– Robert Lewis
Mar 30 at 2:29
$begingroup$
Is there (supposed to be) an equation for $x_2'$? Or, how does $x_2$ evolve? Cheers!
$endgroup$
– Robert Lewis
Mar 30 at 2:29
1
1
$begingroup$
No equation for $x_2'$ unfortunately. $x_2 = u(x)$ would be the control input for this system, and the necessary conditions give this system of equations.
$endgroup$
– Josh Pilipovsky
Mar 30 at 2:33
$begingroup$
No equation for $x_2'$ unfortunately. $x_2 = u(x)$ would be the control input for this system, and the necessary conditions give this system of equations.
$endgroup$
– Josh Pilipovsky
Mar 30 at 2:33
add a comment |
1 Answer
1
active
oldest
votes
$begingroup$
$$begincases
fracdx_1dx = -x_2 \
fracdx_3dx= frac-4x_2^31+x_2^2 \
x_3 = frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
endcases$$
$$fracdx_1dx_3= frac1+x_2^24x_2^2= frac14x_2^2+ frac14 quadimpliesquad frac1x_2^2 =4fracdx_1dx_3-1$$
$$x_3 = frac4x_1(3 frac1x_2^2+1)( frac1x_2^2+1)^2=
frac4x_1(3 (4fracdx_1dx_3-1 )+1)( 4fracdx_1dx_3-1 +1)^2=
frac12 x_1frac6fracdx_1dx_3-1(fracdx_1dx_3)^2$$
$$x_1left(fracdx_3dx_1right)^2 -6x_1fracdx_3dx_1+2x_3=0$$
Or, on a more usual form, with $x_1=X$ and $x_3=Y$ :
$$(Y')^2-6Y'+frac2XY=0$$
This kind of non-linear ODE has no simple general solution.
There is an obvious particular solution : $quad Y=4Xquadimpliesquad x_3=4x_1$ . As a consequence a particular solution of the problem can be found :
$x_3=4x_1=frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
quadimpliesquad x_2=pm 1$
$fracdx_1dx = -x_2=mp 1quad$ and with condition $x_1(0)=a$ :
$$begincasesx_1= mp x+a \
x_2:=pm 1 \
x_3=mp 4x+4a
endcases$$
This an exact solution of the problem if $quad 4x_1(l)=x_3(l)=4amp 4(l)$ .
If $quad 4x_1(l)=x_3(l)neq 4amp 4(l) quad$ I am afraid that there is no closed form solution (made of a finite number of standard functions). Then numerical calculus is required.
$endgroup$
add a comment |
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$begingroup$
$$begincases
fracdx_1dx = -x_2 \
fracdx_3dx= frac-4x_2^31+x_2^2 \
x_3 = frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
endcases$$
$$fracdx_1dx_3= frac1+x_2^24x_2^2= frac14x_2^2+ frac14 quadimpliesquad frac1x_2^2 =4fracdx_1dx_3-1$$
$$x_3 = frac4x_1(3 frac1x_2^2+1)( frac1x_2^2+1)^2=
frac4x_1(3 (4fracdx_1dx_3-1 )+1)( 4fracdx_1dx_3-1 +1)^2=
frac12 x_1frac6fracdx_1dx_3-1(fracdx_1dx_3)^2$$
$$x_1left(fracdx_3dx_1right)^2 -6x_1fracdx_3dx_1+2x_3=0$$
Or, on a more usual form, with $x_1=X$ and $x_3=Y$ :
$$(Y')^2-6Y'+frac2XY=0$$
This kind of non-linear ODE has no simple general solution.
There is an obvious particular solution : $quad Y=4Xquadimpliesquad x_3=4x_1$ . As a consequence a particular solution of the problem can be found :
$x_3=4x_1=frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
quadimpliesquad x_2=pm 1$
$fracdx_1dx = -x_2=mp 1quad$ and with condition $x_1(0)=a$ :
$$begincasesx_1= mp x+a \
x_2:=pm 1 \
x_3=mp 4x+4a
endcases$$
This an exact solution of the problem if $quad 4x_1(l)=x_3(l)=4amp 4(l)$ .
If $quad 4x_1(l)=x_3(l)neq 4amp 4(l) quad$ I am afraid that there is no closed form solution (made of a finite number of standard functions). Then numerical calculus is required.
$endgroup$
add a comment |
$begingroup$
$$begincases
fracdx_1dx = -x_2 \
fracdx_3dx= frac-4x_2^31+x_2^2 \
x_3 = frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
endcases$$
$$fracdx_1dx_3= frac1+x_2^24x_2^2= frac14x_2^2+ frac14 quadimpliesquad frac1x_2^2 =4fracdx_1dx_3-1$$
$$x_3 = frac4x_1(3 frac1x_2^2+1)( frac1x_2^2+1)^2=
frac4x_1(3 (4fracdx_1dx_3-1 )+1)( 4fracdx_1dx_3-1 +1)^2=
frac12 x_1frac6fracdx_1dx_3-1(fracdx_1dx_3)^2$$
$$x_1left(fracdx_3dx_1right)^2 -6x_1fracdx_3dx_1+2x_3=0$$
Or, on a more usual form, with $x_1=X$ and $x_3=Y$ :
$$(Y')^2-6Y'+frac2XY=0$$
This kind of non-linear ODE has no simple general solution.
There is an obvious particular solution : $quad Y=4Xquadimpliesquad x_3=4x_1$ . As a consequence a particular solution of the problem can be found :
$x_3=4x_1=frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
quadimpliesquad x_2=pm 1$
$fracdx_1dx = -x_2=mp 1quad$ and with condition $x_1(0)=a$ :
$$begincasesx_1= mp x+a \
x_2:=pm 1 \
x_3=mp 4x+4a
endcases$$
This an exact solution of the problem if $quad 4x_1(l)=x_3(l)=4amp 4(l)$ .
If $quad 4x_1(l)=x_3(l)neq 4amp 4(l) quad$ I am afraid that there is no closed form solution (made of a finite number of standard functions). Then numerical calculus is required.
$endgroup$
add a comment |
$begingroup$
$$begincases
fracdx_1dx = -x_2 \
fracdx_3dx= frac-4x_2^31+x_2^2 \
x_3 = frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
endcases$$
$$fracdx_1dx_3= frac1+x_2^24x_2^2= frac14x_2^2+ frac14 quadimpliesquad frac1x_2^2 =4fracdx_1dx_3-1$$
$$x_3 = frac4x_1(3 frac1x_2^2+1)( frac1x_2^2+1)^2=
frac4x_1(3 (4fracdx_1dx_3-1 )+1)( 4fracdx_1dx_3-1 +1)^2=
frac12 x_1frac6fracdx_1dx_3-1(fracdx_1dx_3)^2$$
$$x_1left(fracdx_3dx_1right)^2 -6x_1fracdx_3dx_1+2x_3=0$$
Or, on a more usual form, with $x_1=X$ and $x_3=Y$ :
$$(Y')^2-6Y'+frac2XY=0$$
This kind of non-linear ODE has no simple general solution.
There is an obvious particular solution : $quad Y=4Xquadimpliesquad x_3=4x_1$ . As a consequence a particular solution of the problem can be found :
$x_3=4x_1=frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
quadimpliesquad x_2=pm 1$
$fracdx_1dx = -x_2=mp 1quad$ and with condition $x_1(0)=a$ :
$$begincasesx_1= mp x+a \
x_2:=pm 1 \
x_3=mp 4x+4a
endcases$$
This an exact solution of the problem if $quad 4x_1(l)=x_3(l)=4amp 4(l)$ .
If $quad 4x_1(l)=x_3(l)neq 4amp 4(l) quad$ I am afraid that there is no closed form solution (made of a finite number of standard functions). Then numerical calculus is required.
$endgroup$
$$begincases
fracdx_1dx = -x_2 \
fracdx_3dx= frac-4x_2^31+x_2^2 \
x_3 = frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
endcases$$
$$fracdx_1dx_3= frac1+x_2^24x_2^2= frac14x_2^2+ frac14 quadimpliesquad frac1x_2^2 =4fracdx_1dx_3-1$$
$$x_3 = frac4x_1(3 frac1x_2^2+1)( frac1x_2^2+1)^2=
frac4x_1(3 (4fracdx_1dx_3-1 )+1)( 4fracdx_1dx_3-1 +1)^2=
frac12 x_1frac6fracdx_1dx_3-1(fracdx_1dx_3)^2$$
$$x_1left(fracdx_3dx_1right)^2 -6x_1fracdx_3dx_1+2x_3=0$$
Or, on a more usual form, with $x_1=X$ and $x_3=Y$ :
$$(Y')^2-6Y'+frac2XY=0$$
This kind of non-linear ODE has no simple general solution.
There is an obvious particular solution : $quad Y=4Xquadimpliesquad x_3=4x_1$ . As a consequence a particular solution of the problem can be found :
$x_3=4x_1=frac4x_1x_2^2(3+x_2^2)(1+x_2^2)^2
quadimpliesquad x_2=pm 1$
$fracdx_1dx = -x_2=mp 1quad$ and with condition $x_1(0)=a$ :
$$begincasesx_1= mp x+a \
x_2:=pm 1 \
x_3=mp 4x+4a
endcases$$
This an exact solution of the problem if $quad 4x_1(l)=x_3(l)=4amp 4(l)$ .
If $quad 4x_1(l)=x_3(l)neq 4amp 4(l) quad$ I am afraid that there is no closed form solution (made of a finite number of standard functions). Then numerical calculus is required.
answered Mar 30 at 9:19
JJacquelinJJacquelin
45.5k21857
45.5k21857
add a comment |
add a comment |
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2
$begingroup$
Is there (supposed to be) an equation for $x_2'$? Or, how does $x_2$ evolve? Cheers!
$endgroup$
– Robert Lewis
Mar 30 at 2:29
1
$begingroup$
No equation for $x_2'$ unfortunately. $x_2 = u(x)$ would be the control input for this system, and the necessary conditions give this system of equations.
$endgroup$
– Josh Pilipovsky
Mar 30 at 2:33