Riccati equation

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Short description: Type of differential equation


In mathematics, a Riccati equation in the narrowest sense is any first-order ordinary differential equation that is quadratic in the unknown function. In other words, it is an equation of the form y(x)=q0(x)+q1(x)y(x)+q2(x)y2(x) where q0(x)0 and q2(x)0. If q0(x)=0 the equation reduces to a Bernoulli equation, while if q2(x)=0 the equation becomes a first order linear ordinary differential equation.

The equation is named after Jacopo Riccati (1676–1754).[1]

More generally, the term Riccati equation is used to refer to matrix equations with an analogous quadratic term, which occur in both continuous-time and discrete-time linear-quadratic-Gaussian control. The steady-state (non-dynamic) version of these is referred to as the algebraic Riccati equation.

Conversion to a second order linear equation

The non-linear Riccati equation can always be converted to a second order linear ordinary differential equation (ODE):[2] If y=q0(x)+q1(x)y+q2(x)y2 then, wherever q2 is non-zero and differentiable, Substituting v=yq2, then

v=(yq2)=yq2+yq2=(q0+q1y+q2y2)q2+vq2q2=q0q2+(q1+q2q2)v+v2

which satisfies a Riccati equation of the form v=v2+R(x)v+S(x), where S=q0q2 and R=q1+q2q2.

Substituting v=uu, it follows that u satisfies the linear second-order ODE uR(x)u+S(x)u=0 since

v=(uu)=(uu)+(uu)2=(uu)+v2

so that

uu=v2v=SRv=S+Ruu

and hence uRu+Su=0.

Then substituting the two solutions of this linear second order equation into the transformation y=uq2u=q21[log(u)] suffices to have global knowledge of the general solution of the Riccati equation by the formula:[3] y=q21[log(c1u1+c2u2)].

Complex analysis

In complex analysis, the Riccati equation occurs as the first-order nonlinear ODE in the complex plane of the form[4] dwdz=F(w,z)=P(w,z)Q(w,z), where P and Q are polynomials in w and locally analytic functions of z, i.e., F is a complex rational function. The only equation of this form that is of Painlevé type, is the Riccati equation dw(z)dz=A0(z)+A1(z)w+A2(z)w2, where Ai(z) are (possibly matrix) functions of z.

Application to the Schwarzian equation

An important application of the Riccati equation is to the 3rd order Schwarzian differential equation S(w):=(ww)12(ww)2=f which occurs in the theory of conformal mapping and univalent functions. In this case the ODEs are in the complex domain and differentiation is with respect to a complex variable. (The Schwarzian derivative S(w) has the remarkable property that it is invariant under Möbius transformations, i.e. S(aw+bcw+d)=S(w) whenever adbc is non-zero.) The function y=ww satisfies the Riccati equation y=12y2+f. By the above y=2uu where u is a solution of the linear ODE u+12fu=0. Since ww=2uu, integration gives w=Cu2 for some constant C. On the other hand any other independent solution U of the linear ODE has constant non-zero Wronskian UuUu which can be taken to be C after scaling. Thus w=UuUuu2=(Uu) so that the Schwarzian equation has solution w=Uu.

Obtaining solutions by quadrature

The correspondence between Riccati equations and second-order linear ODEs has other consequences. For example, if one solution of a 2nd order ODE is known, then it is known that another solution can be obtained by quadrature, i.e., a simple integration. The same holds true for the Riccati equation. In fact, if one particular solution y1 can be found, the general solution is obtained as y=y1+u Substituting y1+u in the Riccati equation yields y1+u=q0+q1(y1+u)+q2(y1+u)2, and since y1=q0+q1y1+q2y12, it follows that u=q1u+2q2y1u+q2u2 or u(q1+2q2y1)u=q2u2, which is a Bernoulli equation. The substitution that is needed to solve this Bernoulli equation is z=1u Substituting y=y1+1z directly into the Riccati equation yields the linear equation z+(q1+2q2y1)z=q2 A set of solutions to the Riccati equation is then given by y=y1+1z where z is the general solution to the aforementioned linear equation.

See also

References

  1. Riccati, Jacopo (1724) "Animadversiones in aequationes differentiales secundi gradus" (Observations regarding differential equations of the second order), Actorum Eruditorum, quae Lipsiae publicantur, Supplementa, 8 : 66-73. Translation of the original Latin into English by Ian Bruce.
  2. Ince, E. L. (1956), Ordinary Differential Equations, New York: Dover Publications, pp. 23–25 
  3. Conte, Robert (1999). "The Painlevé Approach to Nonlinear Ordinary Differential Equations". The Painlevé Property. New York, NY: Springer New York. pp. 5,98. doi:10.1007/978-1-4612-1532-5_3. ISBN 978-0-387-98888-7. 
  4. Ablowitz, Mark J.; Fokas, Athanassios S. (2003), Complex Variables, Cambridge University Press, p. 184, ISBN 978-0-521-53429-1 

Further reading