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Re: DRSSTC design procedure - draft
Original poster: "Antonio Carlos M. de Queiroz" <acmdq-at-uol-dot-com.br>
Tesla list wrote:
>
> Original poster: "Bob (R.A.) Jones" <a1accounting-at-bellsouth-dot-net>
> Voltage gain(pk out V/square wave input V) =
(8/(Pi*k))*sqrt(Lb/La)
This is the -exact- expression for the mid-frequency case.
> or
> (8/(Pi*k))*sqrt(Ca/Cb)
Close.
> A factor of 4/pi is required to determine the peak amplitude of the
> fundamental of a square wave.
Ok. I forgot this.
> It assumes that (La*s +1/Ca*s+Ra)(Lb*s+1/Cb*s+Rb) << Lab*s, where s
> Laplace operator.
> This is a reasonable assumption when driving at the mid frequency and given
> reasonable Q's (Ra*Rb<<(Lab*s)^2).
> Then transfer function reduces to 1/(Lab*Cb*s^2) substitute k*sqr(La*Lb) for
> Lab
> Then assuming the La*Ca=Lb*Cb (only required to be closer than the split
> frequencies) substitute (La*Ca*Lb*Cb) for s^2 and simplfy.
Why to include Ra?
> At start up there is the steady state response and the transient response
> which are initially equal and opposite and hence cancell. After a number of
> cycles they sum at the output doubling the steady state response (similar to
> the x4 thing with Ca and Cb). So x 2 then x 4/pi for the square wave drive
> factor.
I would say that this happens because the transformer is tuned at both
sides to the same frequency, and the turns ratio is n=sqrt(Lb/La)/k in
the model:
. 1:n
. o--Ca--La(1-k^2)--+ +---+---+
. ) ( | |
. ) ( Lb Cb
. ) ( | |
. o-----------------+ +---+---+
> For the second version we can substitute the ratio of the L's with the ratio
> of the C's.
But it happens that my design doesn't result in this !?
Using the tuning relation CaLa(1-k^2)=LbCb. The gain as function of
the capacitances would be:
Av=(8/pi)*sqrt(Ca/Cb)*sqrt(1/kab^2-1)
And indeed it is, exactly, but only for sinusoidal input. The other
formula works with cosinusoidal input too. Curious.
> Its also useful to note that Vmax(ca)= Vin(4/k*pi) = 6,338V
Works well too.
Antonio Carlos M. de Queiroz