2 - What I've learned so far: Difference between revisions
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<math> e^{j2 \pi nt/T}</math> ->-> <math>\int_{-\infty}^{\infty}e^{j2 \pi nt/T}*h(t-t_0)dt_0</math> |
<math> e^{j2 \pi nt/T}</math> ->-> <math>\int_{-\infty}^{\infty}e^{j2 \pi nt/T}*h(t-t_0)dt_0</math> |
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I hadn't realized the value to this last part until now where by using e it breaks the signal into two easy to manage parts the eigenvector <math> e^{j2 \pi nt/T}</math> and the eigenvalue <h(t)|<math> e^{j2 \pi nt/T}</math>> |
I hadn't realized the value to this last part until now where by using e it breaks the signal into two easy to manage parts the eigenvector <math> e^{j2 \pi nt/T}</math> and the eigenvalue <h(t)|<math> e^{j2 \pi nt/T}</math>> or h(w_n) |
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Revision as of 20:11, 7 October 2009
So far in this class I have expanded my knowledge on "The Game". The Game works for all time invariant systems like this.
In ->->->->->-> Out ->->->Reason
->->->->->h(x) ->->-> Given
Now the more recent
->->
I hadn't realized the value to this last part until now where by using e it breaks the signal into two easy to manage parts the eigenvector and the eigenvalue <h(t)|> or h(w_n)