crossman
Senior Member
- Location
- Southeast Texas
Well Holy Cr@p!
Well Holy Cr@p!
Rattus! :grin:
This is what has been bashing me in the head for the past four hours!!! I knew there was a connection somewhere, I finally figured it out. And you made reference to it up there when you said something to the order of "my way and winnie's way are the same thing. So you were just hinting around, wondering if I would ever figure it out for myself?
I would have done this earlier, but I was trying to pin you down about whether the input and output powers were the same.
Check it out:
You say that the average power of the input to the filter is:
Pt = .636 x Ep x Ip
We're good on that.
I said that the average power at the load would be:
.5 x Ep x Ip ; this comes from .707 x Ep x .707 x Ip
I didn't recognize or have a clue (and still have my doubts:roll: ) that the peak voltage of the fundamental which would pass through the filter would be 4/pi Ep.
So, if we include the increased output voltage of the fundamental in my formula for average power at the load, we get:
4/pi x .5 x Ep x Ip
and since the filter is perfect with no losses, Input power = output power:
Your equation for input power = my equation for output power:
.636 x Ep x Ip = 4/pi x .5 x Ep x Ip
do the algebra, Ep and Ip cancel,
.636 = 4/pi x .5
and it certainly does. That is dadgum beautiful and unexpected. :smile:
So, I will conclude that the "perfect" filter needed for the job above must as a necessity produce a sine wave voltage which has a peak which is a tad bit larger than the peak of the square wave input.
Edit: I just did this with something else you posted:
Vrmsf = Vp x 4/(sqrt(2) x pi) = 0.9Vp
If I substitute this as the voltage in my equation for average power at the output of the filter, everything works out also. Makes sense since it just algebra with the numbers.
Edit again: Winnine, thank you also for your informative posts. I hope you will continue monitoring this thread because I have at least 5 questions I need cleared up.
Well Holy Cr@p!
Rattus! :grin:
This is what has been bashing me in the head for the past four hours!!! I knew there was a connection somewhere, I finally figured it out. And you made reference to it up there when you said something to the order of "my way and winnie's way are the same thing. So you were just hinting around, wondering if I would ever figure it out for myself?
Check it out:
You say that the average power of the input to the filter is:
Pt = .636 x Ep x Ip
We're good on that.
I said that the average power at the load would be:
.5 x Ep x Ip ; this comes from .707 x Ep x .707 x Ip
I didn't recognize or have a clue (and still have my doubts:roll: ) that the peak voltage of the fundamental which would pass through the filter would be 4/pi Ep.
So, if we include the increased output voltage of the fundamental in my formula for average power at the load, we get:
4/pi x .5 x Ep x Ip
and since the filter is perfect with no losses, Input power = output power:
Your equation for input power = my equation for output power:
.636 x Ep x Ip = 4/pi x .5 x Ep x Ip
do the algebra, Ep and Ip cancel,
.636 = 4/pi x .5
and it certainly does. That is dadgum beautiful and unexpected. :smile:
So, I will conclude that the "perfect" filter needed for the job above must as a necessity produce a sine wave voltage which has a peak which is a tad bit larger than the peak of the square wave input.
Edit: I just did this with something else you posted:
Vrmsf = Vp x 4/(sqrt(2) x pi) = 0.9Vp
If I substitute this as the voltage in my equation for average power at the output of the filter, everything works out also. Makes sense since it just algebra with the numbers.
Edit again: Winnine, thank you also for your informative posts. I hope you will continue monitoring this thread because I have at least 5 questions I need cleared up.
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