2 - What I've learned so far: Difference between revisions

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<math>del(x)</math> ->->->->->h(x) ->->-> Given
<math>del(x)</math> ->->->->->h(x) ->->-> Given


Now the more recent
Now the more recent part


<math>e^{j2 \pi nt/T}</math> ->-> <math>\int_{-\infty}^{\infty}x</math>
<math> e^{j2 \pi nt/T}</math> ->-> <math>\int_{-\infty}^{\infty}e^{j2 \pi nt_0/T}h(t-t_0)dt_0</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 <math>h(w_n)</math>

Latest revision as of 16:26, 8 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 part

->->

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