Method of characteristics and second order PDE.

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SUMMARY

The method of characteristics is effectively applied to second order partial differential equations (PDEs), specifically hyperbolic equations like utt = uxx - 2ut. The characteristic equation derived from this PDE is t² = x², leading to the characteristics t - x = constant and t + x = constant. By substituting p = t - x and q = t + x, the equation simplifies, allowing for the transformation of derivatives using the chain rule. This results in a simplified form that reveals the relationship 4u_{pq} = u_p + u_q.

PREREQUISITES
  • Understanding of partial differential equations (PDEs)
  • Familiarity with the method of characteristics
  • Knowledge of chain rule in calculus
  • Basic concepts of hyperbolic equations
NEXT STEPS
  • Study the method of characteristics in detail for various types of PDEs
  • Explore hyperbolic equations and their properties
  • Learn about the chain rule applications in multivariable calculus
  • Investigate numerical methods for solving second order PDEs
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Mathematicians, physicists, and engineers working with partial differential equations, particularly those focusing on hyperbolic equations and their applications in modeling wave phenomena.

peripatein
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This isn't a homework question per se. Am merely seeking an explanation how the method of characteristics may be applied to a second order PDE. For instance, how is it used to solve utt=uxx-2ut?
 
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That is a "hyperbolic" equation and, ignoring the lower order, first derivative is u_{tt}= u_{xx} so has "characteristic equation"t^2= x^2 or t= \pm x so the "characteristics" are t- x= constant or t+ x= constant.

That tells us that we can simplify the equation by taking p= t- x and q= t+ x as variables instead of x and t. By the chain rule, u_t= u_pp_t+ u_qq_t= u_p+ u_q and then u_{tt}= (u_p+ u_q)_t= (u_p+ u_q)_p+ (u_p+ u_q)_q= u_{pp}+ 2u_{pq}+ u_{qq}.

Similarly, u_x= u_pp_x+ u_qq_x= -u_p+ u_q and then u_{xx}= (-u_p+ u_q)_x= -(-u_p+ u_q)_p+ (-u_p+ u_q)_q= u_pp- 2u_{pq}+ u_{qq}.

So u_{tt}= u_{xx}+ u_t becomes u_{pp}+ 2u_{pq}+ u_{qq}= u_pp- 2u_{pq}+ u_{qq}+ u_p+ u_q. The "u_{pp}" and "u_{qq}" cancel, leaving 4u_{pq}= u_p+ u_q.
 

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