Hi Karel,
Yes, correct screen (and cathode) bypassing is a real 'gedoente'. It is easily done with formulae as per RDH (IV) p. 496 - 501 and elsewhere .... but impossible because one does not have the parameters needed there.
Technical Content:
Perhaps of general interest: One starts with the basic relationship of "R = 2.pi.ƒ.C" (what is the keybord code for pi?), but when bypassing active elements, there of course needs to be an increase in C because of amplification involved, rather like with the Miller effect. Thus R.g2-C of 1 megohm and 10nF will give a passive -3dB point at 16Hz, but using it on G2 of an EF86 will raise that frequency to over 40Hz because there is gain from G2 to anode.
Here I chicken out and use the engineering way. It is easier to hook the circuit up with the specific components and measure with a signal generator, changing C until one has what is wanted (and tabulate the results for future reference).
Per basics the screen is bypassed to cathode (viz. a 'common cathode' topology). This will be the same as taking it to earth when the cathode is properly bypassed. For those looking at the phase effect (important in l.f. stability in amplifiers with NFB), it is useful to realise that phase shift initially caused returns to zero at very low frequency where capasitive reactance become large. THis can be a handy 'tool' to keep l.f. stability within bounds.
In the classic power amplifier topology where NFB is applied to the first stage cathode the screen bypass is returned to the cathode and not earth, so as to preserve a pentode configuration in the first stage. In some designs this is overlooked, giving a funny kind of 'tapped screen' topology, which I have not done measurements on yet. I would believe that that is counter-indicated, seeing as how the NFB-signal is dumped on the input stage with power stage distortion (higher then the rest) in series with the screen.
In your case with the SRPP, Karel, the situation is of course different.