Characteristic method + Jacobian

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SUMMARY

The discussion centers on the application of the method of characteristics to solve a first-order semi-linear partial differential equation (PDE) represented by the equation x∂ψ/∂x + t∂ψ/∂t + (x + 2t)ψ = 3xt with the initial condition ψ(x, 4x) = x. The Jacobian determinant |∂(x,t)/∂(σ,η)| being zero indicates that the characteristic curves are colinear with the initial condition, leading to the conclusion that a solution cannot be constructed. This results in the inability to define a well-posed solution due to the normal vector for the parametrized surface being zero.

PREREQUISITES
  • Understanding of first-order semi-linear partial differential equations (PDEs)
  • Familiarity with the method of characteristics
  • Knowledge of Jacobian determinants and their implications
  • Ability to interpret initial conditions in the context of PDEs
NEXT STEPS
  • Study the method of characteristics in detail, focusing on its application to first-order PDEs
  • Learn about Jacobian determinants and their role in determining the existence and uniqueness of solutions
  • Explore examples of initial conditions that lead to well-posed problems in PDEs
  • Investigate alternative methods for solving PDEs when characteristics are colinear with initial conditions
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Mathematicians, physicists, and engineers working with partial differential equations, particularly those interested in the method of characteristics and the implications of Jacobian determinants on solution existence and uniqueness.

nicksauce
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If I am using the method of characteristics to solve a PDE \Psi(x,t) (first order, semi-linear), and after using the method of characteristics I find that the Jacobian
|\frac{\partial{(x,t)}}{\partial{(\sigma,\eta)}}| = 0
(where \sigma and \eta are parameters for the curve) does this imply that no solution exists, or just that the solution is not unique? I could not find this in my textbook.
 
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Could you post the problem please?
 
Sure.

x\frac{\partial\psi}{\partial{x}} + t\frac{\partial\psi}{\partial{t}} + (x + 2t)\psi = 3xt \textnormal{ With intitial Condition:} \psi (x,4x)=x

This leads me to:

<br /> x(\sigma,\eta) = \eta e^{\sigma}
<br /> t(\sigma,\eta) = 4\eta e^{\sigma}

(I can fill in those steps if necessary too)
 
No, that won't be necesary. The problem is that your initial contidion is over a characteristic, and you can't construct a solution. Remember that the method of characteristics uses the initial condition as curve of departure (parametrized by \eta) and then tries to move further from it as far as the ode system allows it (parametrized by \sigma). In your case, this can't be done, as the characteristic is colinear with the initial condition, which means the normal vector for the parametrized surface is zero (so the surface is not well defined).

Let me give it a little more tought, and i'll get back to you.
 
Last edited:

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