- #1
AbigailM
- 46
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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 [itex]z(t) = Ce^{i \omega t}[/itex]. When we sub in z and it's derivatives we then rewrite the complex constant C as [itex]Ae^{-i \delta}[/itex]. My book says that we can do this for any complex number. Why is this?
When we solve for A and sub that into [itex]C=Ae^{-i \delta}[/itex] we find
[itex]f_{0}e^{i \delta}=A(\omega_{0}^{2} - \omega^{2} +2i \beta \omega)[/itex].
My book says we can then rewrite [itex]\delta[/itex] as [itex]\delta=tan^{-1}\left(\frac{2\beta\omega}{\omega_{0}^{2}-\omega^{2}}\right)[/itex]. 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 [itex]z(t) = Ce^{i \omega t}[/itex]. When we sub in z and it's derivatives we then rewrite the complex constant C as [itex]Ae^{-i \delta}[/itex]. My book says that we can do this for any complex number. Why is this?
When we solve for A and sub that into [itex]C=Ae^{-i \delta}[/itex] we find
[itex]f_{0}e^{i \delta}=A(\omega_{0}^{2} - \omega^{2} +2i \beta \omega)[/itex].
My book says we can then rewrite [itex]\delta[/itex] as [itex]\delta=tan^{-1}\left(\frac{2\beta\omega}{\omega_{0}^{2}-\omega^{2}}\right)[/itex]. Could someone please explain this? The right triangle explanation is confusing me.
Thank you all.