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#31 | |
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diyAudio Member
Join Date: Dec 2012
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Quote:
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#32 |
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diyAudio Member
Join Date: Dec 2012
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Gootee, thanks very much for taking the time to write up that long, detailed post.
I'm going to read through it carefully and digest it all later tonight.
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#33 | |
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diyAudio Member
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But it seems to be a commonly-used shorthand for Watts that are calculated using Volts RMS. According to Wikipedia, in the USA the term for that (i.e. Watts calculated from Vrms squared divided by R) should be "Continuous Power", which was specified in the Federal Trade Commision;s "1974 Amplifier Rule", so that advertising claims for audio amplifier "power" specs would all have to use the same type of measurement (Vrms is measured, using a specified load resistance, at a specified maximum THD value, which usually occurs just before the onset of clipping, and then CP rating = Vrms^2 / R). However, for a purely resistive load, if you multiply Vrms x Irms (Volts RMS time Amps RMS, or, equivalently, calculate Vrms^2 / R or Irms^2 x R), you get the AVERAGE (aka "continuous average") power, in Watts, which, if a sine wave is used, also happens to be one-half of the PEAK SINE Power (also in Watts). Anyway, for a sine wave and a purely-resistive load: Pavg = (Vrms)^2 / R = (Irms)^2 x R = (Vpeak)^2 / (2R) Actual "Peak Power", sometimes also called PMOP (Peak Music Output Power), does NOT have to refer to power while using a sine signal. So it can be many times higher than the Continuous Power rating (typically 5 or 6 times higher). Last edited by gootee; 2nd January 2013 at 10:30 PM. |
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#34 |
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diyAudio Member
Join Date: Nov 2003
Location: Brighton UK
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Hi,
Watts RMS is extremely well defined and not at all obscure. The only issue being it assumes purely resistive loads. Which speakers aren't, but that does not matter. Best to assume speakers are as onerous a load (due to reactance) as half the claimed impedance as resistance. rgds, sreten.
__________________
There is nothing so practical as a really good theory - Ludwig Boltzmann When your only tool is a hammer, every problem looks like a nail - Abraham Maslow Last edited by sreten; 2nd January 2013 at 10:40 PM. |
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#35 |
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diyAudio Member
Join Date: Sep 2012
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could I use a 30ohm resistor across the input to decrease gain and noise? I know it will put a small load across the computers output but it shouldn't be too much right?
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#36 | |
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diyAudio Member
Join Date: Dec 2012
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#37 |
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diyAudio Member
Join Date: Dec 2012
Location: Bucuresti
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about the optical ilussion,it happened to me that the speakers started to move very much in and out while plaiyng music composed of mostly vocals at high levels,the voice is composed of 400hz with variyng amplitudes and the top of the peaks drive the speaker up and down slowly lookin like they ding 1-0.1 hz
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#38 | |
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diyAudio Member
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Quote:
If you want less overall gain, you could use two resistors, to make a voltage divider. That way, you could select 'reasonable" R values but still make the gain of the divider be almost whatever you want. You would need one R in series with the input and one from the input to ground. If you call them Rs and Rg, they would make V_input_pin = Vin x (Rg / (Rg + Rs)). So, for example, to cut the signal in half, you could use two equal-valued resistors. Your blocking capacitor would see Rs+Rg to ground, I think. So you can calculate the Rs+Rg needed to keep your cutoff frequncy down around 1 Hz or less. For 4.7 uF and 1 Hz, for example, Rtotal = 1 / (2 x 3.14 x 1 x .0000047) = about 33,900 = 33.9 kOhms, so anything above about 34k total would be fine. Then you would just need to find two R values that give the fractional gain you want, but still add up to at least 34k. (NOTE that if you were installing an actual volume control, which would vary the total resistance whenever the volume was changed, you would want it AHEAD of your capacitor. Otherwise, changing the volume would also change the cutoff frequency of the high-pass filter.) Last edited by gootee; 3rd January 2013 at 04:02 PM. |
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#39 | |
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diyAudio Member
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But, regarding your question: There is not really such a thing as "ground" (or at least there doesn't need to be, for circuits). It's just a convenient concept. There are only loops, where current flows. Whenever the source tries to push electrons out of one of the two wires, it is also trying to pull them in through the other wire. If electrons do go out through one of the source's output wires, then they must also come in through the other wire, at exactly the same rate, unless there is some other path they could follow, to get all the way back to where the other wire connects to the source. But that would be a "ground loop", which we hope doesn't exist. Last edited by gootee; 3rd January 2013 at 04:06 PM. |
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#40 | |
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diyAudio Member
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If not, all electrons would accumulate at one point and we would run out of electrons, eventually ![]() If you're really interested (which I doubt) you might Google Thevenin (which says all voltages in a loop sum to zero) or Norton (all currents in a node sum to zero). jan
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/Yes! Its out: Linear Audio Vol 5! I'm not an "accademic", just a plodder who loves a challenge - Ian Hegglun |
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