数学物理学报(英文版) ›› 1993, Vol. 13 ›› Issue (1): 65-73.

• 论文 • 上一篇    下一篇

GLOBAL C1 SOLUTION OF CAUCHY PROBLEM FOR TWO-DIMENSIONAL GAS DYNAMICS SYSTEM

陆云光   

  1. Inst. of Math. Sci., Academia Sinica, Wuhan 430071, China
  • 收稿日期:1991-05-28 出版日期:1993-03-25 发布日期:1993-03-25

GLOBAL C1 SOLUTION OF CAUCHY PROBLEM FOR TWO-DIMENSIONAL GAS DYNAMICS SYSTEM

Lu Yunguang   

  1. Inst. of Math. Sci., Academia Sinica, Wuhan 430071, China
  • Received:1991-05-28 Online:1993-03-25 Published:1993-03-25

摘要: Using the method of characteristic lines this paper considers the global C1 solution of the Cauchy problem for two-dimensional gas dynamics system. When the initial data degenerate to the special case ρ0(x, y)=const, the global C1 solution is obtained. For the case of isentropic exponent γ=1, a transformation about variables is introduced, which changes the system to a first order linear hyperbolic system with constant coefficients and the global C1 solution is also obtained in this case when the initial data of the forms (ρ0(x, y), u0(x, y), v0(x, y))=(exp(ω01 (c1x+d1y)+ω02(c2x+d2y)), u01(c1x+d1y)+u02(c2x+d2y), u01(c1x+d1y)+u02(c2x+d2y)), where ci and di(i=1, 2) are constants.

Abstract: Using the method of characteristic lines this paper considers the global C1 solution of the Cauchy problem for two-dimensional gas dynamics system. When the initial data degenerate to the special case ρ0(x, y)=const, the global C1 solution is obtained. For the case of isentropic exponent γ=1, a transformation about variables is introduced, which changes the system to a first order linear hyperbolic system with constant coefficients and the global C1 solution is also obtained in this case when the initial data of the forms (ρ0(x, y), u0(x, y), v0(x, y))=(exp(ω01 (c1x+d1y)+ω02(c2x+d2y)), u01(c1x+d1y)+u02(c2x+d2y), u01(c1x+d1y)+u02(c2x+d2y)), where ci and di(i=1, 2) are constants.