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Hi,
I am going through the problems from "Signals and Systems" by Alan V.
Oppenheim et. al. and I found this problem:
To determine if x(t) is periodic and to find it's period if it is,
where x(t) is:
x(t) = SIGMA (e^(-2t-n)) where n varies from minus infinity to plus
infinity.
Now, as far as I can tell 'e' raised to anything that isn't a complex
quantity is not going to be periodic. Therefore, I concluded that x(t)
as defined above is not periodic.
But then, I just can't tell what type of a signal this is. Too many
things that confuse me:
1. For a given value of t, does the summation converge to a neat
value or does it diverge?
2. This mix of a continuous ('t') and discrete ('n') variable! Never
seen something like this.
3. I wonder if this is a twisted representation of some
familiar/popular/classic/obvious function.
What do you think?
Regards,
Anand
______________________________Am 28.06.2012 21:07, schrieb Anand P. Paralkar:
> Hi,
>
> I am going through the problems from "Signals and Systems" by Alan V.
> Oppenheim et. al. and I found this problem:
>
> To determine if x(t) is periodic and to find it's period if it is, where
> x(t) is:
>
> x(t) = SIGMA (e^(-2t-n)) where n varies from minus infinity to plus
> infinity.
Do you mean
\sum_{n=-\infty}^\infty e^{-2t - n}
and are you sure that you haven't forgotten a square somewhere in the
exponent, as in
\sum_{n=-\infty}^\infty e^{-(t - n)^2} ?
For the former, use the functional relation of the exponential to write
it as
.. = e^{-2t} \sum_{n=-\infty}^\infty e^{-n}
where the latter sum clearly does not converge because -n->\infty as
n->\infty and thus the sum explodes.
So this function is not defined. The latter sum, however, with the ^2 in
the exponent, does converge for every t, it is actually absolutely
convergent - it is bounded by the geometric series, and converges
independent of t, so the limit is also continuous (actually, even
smooth). It is obviously periodic with period one (substitute n->n+1).
In fact, with a little substitution, you see that this is up to a phase
just a special case of the theta function:
http://en.wikipedia.org/wiki/Theta_function
which is a complex function which is "as periodic" as a holomorphic
function could ever be (periodic in one direction, periodic up to a
phase in the second).
HTHH,
Thomas
______________________________Hi, probably it's a typo and the idea is that a sum c_k exp(i omega k t) over k = any set of integers is periodic in 1/omega. If so, each term is periodic on its own, so there is IMO not much left to prove. But I'm guessing on the nature of the question, so I may be completely wrong.______________________________
What's the problem number? Here's the solution manual to the 2nd edition: http://www.scribd.com/doc/13377530/Signals-and-Systems-2E-Oppenheim-Solutions______________________________
Hi Thomas,
Thanks for your reply. I checked the book again, I don't think I have
forgotten a square. I must however point-out that the first expression
given in your reply should actually be:
SIGMA(e^(-(2t-n)))
not:
SIGMA(e^(-2t-n))
In either case, I am unable to make out anything of what's happening to
the shape of the signal.
The reason why I posted this question is that this book has a learning
at every possible nook and corner. I am surprised to see a function
that "leads to nowhere".
Thanks so much for looking into this,
Anand
On 29-06-2012 01:31, Thomas Richter wrote:
> Am 28.06.2012 21:07, schrieb Anand P. Paralkar:
>> Hi,
>>
>> I am going through the problems from "Signals and Systems" by Alan V.
>> Oppenheim et. al. and I found this problem:
>>
>> To determine if x(t) is periodic and to find it's period if it is, where
>> x(t) is:
>>
>> x(t) = SIGMA (e^(-2t-n)) where n varies from minus infinity to plus
>> infinity.
>
> Do you mean
>
> \sum_{n=-\infty}^\infty e^{-2t - n}
>
> and are you sure that you haven't forgotten a square somewhere in the
> exponent, as in
>
> \sum_{n=-\infty}^\infty e^{-(t - n)^2} ?
>
> For the former, use the functional relation of the exponential to write
> it as
>
> .. = e^{-2t} \sum_{n=-\infty}^\infty e^{-n}
>
> where the latter sum clearly does not converge because -n->\infty as
> n->\infty and thus the sum explodes.
>
> So this function is not defined. The latter sum, however, with the ^2 in
> the exponent, does converge for every t, it is actually absolutely
> convergent - it is bounded by the geometric series, and converges
> independent of t, so the limit is also continuous (actually, even
> smooth). It is obviously periodic with period one (substitute n->n+1).
> In fact, with a little substitution, you see that this is up to a phase
> just a special case of the theta function:
>
> http://en.wikipedia.org/wiki/Theta_function
>
> which is a complex function which is "as periodic" as a holomorphic
> function could ever be (periodic in one direction, periodic up to a
> phase in the second).
>
> HTHH,
> Thomas
______________________________:) The problem number is 1.25 (f). I tried the solution manual. It has a terse "Not periodic". There is an answer but no answer there! :) Regards, Anand On 29-06-2012 19:46, David Drumm wrote: > What's the problem number? > > Here's the solution manual to the 2nd edition: > > http://www.scribd.com/doc/13377530/Signals-and-Systems-2E-Oppenheim-Solutions______________________________