Jacobi elliptic functions with complex variables

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SUMMARY

The discussion focuses on solving the Duffing's equation ##\ddot{x}(t)+\alpha x(t)+\beta x^3(t)=0##, where ##\alpha## is a complex number with ##Re \alpha<0## and ##\beta>0##. The solution involves Jacobi elliptic functions, specifically ##cn(\omega t,k)##, where both ##\omega## and ##k## are complex. The key challenge is addressing the complexity of ##k##, particularly in the context of the function ##cn(z_1+iz_2, k_1+i k_2)##. The discussion suggests utilizing the definition of elliptic functions in terms of theta functions and applying series inversion to convert the elliptic modulus to the ##\tau## modulus.

PREREQUISITES
  • Understanding of Duffing's equation and its parameters
  • Familiarity with Jacobi elliptic functions and their properties
  • Knowledge of complex analysis, particularly with complex variables
  • Experience with theta functions and their applications in elliptic functions
NEXT STEPS
  • Study the properties of Jacobi elliptic functions and their complex arguments
  • Learn about the series inversion method for elliptic functions
  • Explore the relationship between complex frequency and amplitude in oscillatory systems
  • Investigate the application of theta functions in solving elliptic equations
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Mathematicians, physicists, and engineers working on nonlinear dynamics, particularly those dealing with complex systems and elliptic functions in differential equations.

karlzr
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I am trying to solve a Duffing's equation ##\ddot{x}(t)+\alpha x(t)+\beta x^3(t)=0## where ##\alpha## is a complex number with ##Re \alpha<0## and ##\beta>0##. The solution can be written as Jacobi elliptic function ##cn(\omega t,k)##. Then both ##\omega## and ##k## are complex. The solution to ##\omega## being complex can found from textbooks. So my question is how to deal with ##k## being complex?

How to deal with ##cn(z_1+iz_2, k_1+i k_2)## where ##z_i## and ##k_i## are real numbers?

In the case of harmonic oscillator, imaginary part of the frequency square will change the amplitude of oscillator just like what friction terms do. I am wondering whether we have similar equivalence in this case?

Thanks for your time!
 
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karlzr said:
I am trying to solve a Duffing's equation ##\ddot{x}(t)+\alpha x(t)+\beta x^3(t)=0## where ##\alpha## is a complex number with ##Re \alpha<0## and ##\beta>0##. The solution can be written as Jacobi elliptic function ##cn(\omega t,k)##. Then both ##\omega## and ##k## are complex. The solution to ##\omega## being complex can found from textbooks. So my question is how to deal with ##k## being complex?

How to deal with ##cn(z_1+iz_2, k_1+i k_2)## where ##z_i## and ##k_i## are real numbers?

In the case of harmonic oscillator, imaginary part of the frequency square will change the amplitude of oscillator just like what friction terms do. I am wondering whether we have similar equivalence in this case?

Thanks for your time!

I think you want to use the definition of elliptic functions in term of theta functions. You must use a series inversion described there to convert the elliptic modulus to the ##\tau## modulus.
 

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