Tzitzeica equation

The Tzitzeica equation is a nonlinear partial differential equation devised by Gheorghe Țițeica in 1907 in the study of differential geometry, describing surfaces of constant affine curvature.[1] The Tzitzeica equation has also been used in nonlinear physics, being an integrable 1+1 dimensional Lorentz invariant system.[2]

u_{xy}=\exp(u)-\exp(-2*u).

On substituting

w(x, y) = exp(u(x, y))

the equation becomes

 w(x, y)_{y, x}*w(x, y)-w(x, y)_{x}*w(x, y)_{y}-w(x, y)^3+1 = 0

Obtain the traveling solution of the original equation by the reverse transformation u(x,y)=ln(w(x,y)).


Analytic solution

Some elementary solutions have the general form of ln(a*f(bx+cy+d));where a,b,c,d are arbitrary constants,and where f is one of: sec,csc,coth,tanh,tan.

u(x, y)=ln( -1/2-(1/2*I)*\sqrt(3)+(3/4+(3/4*I)*\sqrt(3))*csc(_C1+_C2*x+(3/4)*(1/2+(1/2*I)*\sqrt(3))*y/_C2)^2)
u(x, y) =ln( -1/2-(1/2*I)*\sqrt(3)+(3/4+(3/4*I)*\sqrt(3))*sec(_C1+_C2*x+(3/4)*(1/2+(1/2*I)*\sqrt(3))*y/_C2)^2)
u(x, y) =ln( -1/2+(1/2*I)*\sqrt(3)+(3/4-(3/4*I)*\sqrt(3))*csc(_C1+_C2*x+(3/4)*(1/2-(1/2*I*\sqrt(3))*y/_C2)^2)
u(x, y) =ln(1/4-(1/4*I)*\sqrt(3)+(-3/4+(3/4*I)*\sqrt(3))*coth(_C1+_C2*x+(3/4)*(-1/2+(1/2*I)*sqrt(3))*y/_C2)^2)
u(x, y) = ln(1/4-(1/4*I)*\sqrt(3)+(-3/4+(3/4*I)*\sqrt(3))*tanh(_C1+_C2*x+(3/4)*(-1/2+(1/2*I)*sqrt(3))*y/_C2)^2)
u(x, y) =ln( 1/4-(1/4*I)*\sqrt(3)+(3/4-(3/4*I)*\sqrt(3))*cot(_C1+_C2*x+(3/4)*(1/2-(1/2*I)*\sqrt(3))*y/_C2)^2)
u(x, y) =ln( 1/4-(1/4*I)*\sqrt(3)+(3/4-(3/4*I)*\sqrt(3))*tan(_C1+_C2*x+(3/4)*(1/2-(1/2*I)*\sqrt(3))*y/_C2)^2)

References

  1. G. Tzitz´eica, “Geometric infinitesimale-sur une nouvelle classes de surfaces,”Comptes Rendus de l’Acad´emie des Sciences, vol. 144, pp. 1257–1259, 1907.
  2. Andrei D. Polyanin,Valentin F. Zaitsev, HANDBOOK OF NONLINEAR PARTIAL DIFFERENTIAL EQUATIONS, SECOND EDITION p540-542 CRC PRESS

Additional reading