[Lowfer] Epson Question

Bill Ashlock [email protected]
Tue, 20 Apr 2004 17:16:23 -0400


Johan,

Thank you for pointing out the error of my ways in the amplitude of the 
square wave fundamental freq. This makes a lot of sense in my calculations 
for the loop current when the input power is known. The measured value was 
always greater than the calculated value. I just located my college textbook 
and, sure enough, there's a 4/pi factor in front of the fourier series!

Bill A


>From: "Johan Bodin" <[email protected]>
>Reply-To: [email protected]
>To: <[email protected]>
>Subject: Re: [Lowfer] Epson Question
>Date: Tue, 20 Apr 2004 07:20:26 -0000
>
>Hi
>
>the fundamental frequency component of a square wave
>has an amplitude of:
>
>Vsine_rms = Vsq_wave_peak_to_peak * square_root (2) / pi
>
>which means
>
>Vsine_rms = Vsq_wave_peak_to_peak * 0.4502
>
>or
>
>Vsine_peak_to_peak = Vsq_wave_peak_peak * 1.2732
>
>(Assuming 50/50 % square wave duty cycle)
>
>Although it may appear surprising, the Vpp of the fundamental
>frequency component is larger than the Vpp of the square wave itself :-)
>
>To run class D, you can put a series resonant circuit of sufficient
>loaded Q, say 5 or more, between the square wave generator and
>the load (XC = XL = 5*Rload, or more).
>
>The series circuit will pass only the fundamental frequency so the
>generator will see only negligible loading on the harmonics.
>This is much better than using a "grounded C input" lowpass
>filter directly at the generator output (which will cause high current
>switching spikes = more switching loss).
>
>BTW, I would guess that the Epson oscillator has a quite "weak" output
>stage so it will probably deliver more power into a load >50 ohms.
>
>73
>Johan SM6LKM
>
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