What is the solution for the attached equation?

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SUMMARY

The equation I(z) = cosh(1/2 ∫I(z)dz) can be approached by deriving both sides with respect to z, leading to an ordinary differential equation. Introducing J(z) = sinh(1/2 ∫I(z)dz) transforms the problem into a two-dimensional system defined by I' = 1/2 IJ and J' = 1/2 I^2, which can be solved numerically with appropriate initial conditions. Alternatively, power series can be constructed iteratively using the recurrence relations I_{n+1}(z) and J_{n+1}(z) based on initial values I(0) and J(0).

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eahaidar
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Good afternoon,
i was just wondering if this equation is possibly solvable where I(z) is a function of z. The equation is:
I(z)=cosh(1/2 ∫I(z)dz)
I know it looks stupid but is it possible? How would you approach this problem?
Thank you.
 

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Try to derive both side with respect to z. This will give you an ordinary differential equation. Then try to solve it in another way.
 
Thanks for the response. However I get hyperbolic sinh which just makes it much worse. :(
 
Maybe first set $$arcosh(I(z))=\frac {1}{2} \int_z^L I(x)dx $$ and then take the derivate?
 
eahaidar said:
Thanks for the response. However I get hyperbolic sinh which just makes it much worse. :(

If you introduce J(z) = \sinh\left(\frac12 \int I(z)\,dz\right) then you can get the two-dimensional system <br /> I&#039; = \frac12 IJ \\<br /> J&#039; = \frac12 I^2<br /> which can be solved numerically subject to given initial conditions (which, like cosh and sinh, must satisfy I(0)^2 - J(0)^2 = 1). Alternatively, you can construct power series iteratively by starting with I_0(z) = I(0), J_0(z) = J(0) and using the recurrence relation <br /> I_{n+1}(z) = I(0) + \frac12 \int_0^z I_n(t)J_n(t)\,dt, \\<br /> J_{n+1}(z) = J(0) + \frac12 \int_0^z I_n^2(t)\,dt.
 

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