AbigailM
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Just have a few questions regarding the method of solving the damped-driven harmonic oscillator.
Once we have rewritten the differential equation in terms of z and it's derivatives, we try a solution z(t) = Ce^{i \omega t}. When we sub in z and it's derivatives we then rewrite the complex constant C as Ae^{-i \delta}. My book says that we can do this for any complex number. Why is this?
When we solve for A and sub that into C=Ae^{-i \delta} we find
f_{0}e^{i \delta}=A(\omega_{0}^{2} - \omega^{2} +2i \beta \omega).
My book says we can then rewrite \delta as \delta=tan^{-1}\left(\frac{2\beta\omega}{\omega_{0}^{2}-\omega^{2}}\right). Could someone please explain this? The right triangle explanation is confusing me.
Thank you all.
Once we have rewritten the differential equation in terms of z and it's derivatives, we try a solution z(t) = Ce^{i \omega t}. When we sub in z and it's derivatives we then rewrite the complex constant C as Ae^{-i \delta}. My book says that we can do this for any complex number. Why is this?
When we solve for A and sub that into C=Ae^{-i \delta} we find
f_{0}e^{i \delta}=A(\omega_{0}^{2} - \omega^{2} +2i \beta \omega).
My book says we can then rewrite \delta as \delta=tan^{-1}\left(\frac{2\beta\omega}{\omega_{0}^{2}-\omega^{2}}\right). Could someone please explain this? The right triangle explanation is confusing me.
Thank you all.