What you are describing sounds a bit like a description of thunder: a sharp,
wideband pulse followed by reverberant randomness, (though not spectrally flat
due to environmental absorption).
Perhaps you can use that as a model?
David Reaves
Recklinghausen, Germany
On Wed, 27 Jul 2016 19:00:02
Perhaps it would be as well for the unsubscribe function on the list
management page to be parked behind a password, rather than accessible
without? At the moment, anyone can do this kind of drive-by
unsubscription of anyone whose email address they have, without even
going to the trouble of
This kind of unsubscribe abuse is unfortunately difficult
to handle. Password protected unsubscribe fails because
geniune unsubscribers almost always forget their password.
I started to look at the GNU Mailman documentation.
There are some options to discuss with both Doug and Robert.
Meanwhile
On 28/07/2016 3:00 AM, gm wrote:
I want to create a signal thats similar to a reverberant knocking or
impact sound,
basically decaying white noise, but with a more compact onset similar to
a minimum phase signal
and spectrally completely flat.
Maybe consider mixing multiple signals together:
Or a captcha, for that matter?
> On 28 Jul 2016, at 10:40, gwenhwyfaer wrote:
>
> Perhaps it would be as well for the unsubscribe function on the list
> management page to be parked behind a password, rather than accessible
> without? At the moment, anyone can do this
> Because I don't think there can be more than one between any two
> adjacent sampling times.
>
>
> This really got the gears turning. It seems true, but is it a theorem?
> If not, can anyone give a counterexample?
>
I don't know whether it's a classical theorem, but I think it is true.
On Wed, Jul 27, 2016 at 10:33:40PM +0200, gm wrote:
> [...]
> So my question for now is: how can we synthesize completely flat
> decaying noise?
> (is it even possible?)
I think the modulation between expdec and white noise is ok:
T = 1 / samplerate
p = exp(log(0.001) * T / t60)
y = (1 -
sorry, that's a decay, so out is "(1 - y) * rand()":
T = 1 / samplerate
p = exp(log(0.001) * T / t60)
y = 1 + p*(y1 - 1)
y1 = y
out = (1 - y) * rand(-1.0, 1.0) * gain
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Haha, Ross, I'm not sure I'll be going *quite* so deep just yet.
My most pressing need is simply to access more processing power than one
callback will give me (without underflow). To that end, I'll be setting up
a signaling system whereby one stream can have "helper threads" that are
notified
Following the comments regarding the exponential
modulated noise segment;
My experience is that all such actual segments will be
spectrally coloured, because of course they contain
a truncated set of random values.
The only theoretically "flat" exciter is the Dirac impulse.
But because it
I used both the minimum phase version of a band limited impulse and also
the "empty" exp curve
the exp decay curve has more energy towards DC depending on its witdh
but you dont hear that
like the "empty" exponential decay segment and dirac impulse the minimum
phase pulse lacks
My problem was that a short segment of random isn't spectrally
straigh-line flat.
If you feed this into a resonator (waveguide) you can hear a difference
between one random grain and another with another random sequence.
This is usally a desired effect that makes the sound alive,
but in my
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