Jacobi elliptic functions with complex variables

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The discussion revolves around solving Duffing's equation with complex parameters, specifically focusing on the Jacobi elliptic function solution, ##cn(\omega t, k)##, where both ##\omega## and ##k## are complex. The user seeks guidance on handling the complex modulus ##k##, particularly in the context of the function ##cn(z_1 + iz_2, k_1 + ik_2)##. It is noted that the imaginary part of the frequency square affects the oscillator's amplitude, akin to friction. A suggestion is made to utilize the definition of elliptic functions in terms of theta functions and to apply a series inversion to convert the elliptic modulus to the ##\tau## modulus. This approach may help in addressing the complexities of the problem.
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.
 
Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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