The 2n5551 has a lower gain than the BC549....and has a higher noise figure. Not sure whther either of those charateristics will affect the result in this application?
The inclusion or R3 and the 'Q' of T1 tends to ensure the oscillator output is pretty linear, in my experience --- although that tends to be relying on the visual oscilloscope representation of the waveform, rather than being able to measure distortion accurately at 10MHz !
I haven't noticed any particular LF lift. I don't have the facility to measure LF response very accurately, and tend to rely on comparative readings.
I normally use my Rode NT1 (black version) as a reference, when doing that.
I don't know whether the fact that - in theory anyway - the LF limit of an RF mic is DC has any impact?
I realise thats not actually true in practice, but there maybe more LF than one might expect from a conventional LDC impedance converter? ...
I have encountered quite a few variations in my experiments using different capsules, oscillator frequencies and capsules....
There have been 2 types of Spectrum '5.3uH' coils....
• The earlier ones -- marked '5R3' - tended to work best with 90pF capsules when used with an 8MHz oscillator.
• The later (current) ones are marked '5u3H' and seem to work better with a 10MHz oscillator, even wth higher value capsules.
The value of C4 needs to be fairly close to the capsule value..
I have had examples where there are several 'peaks' within the inductor tuning range, although there always seem to be a dominant 'peak' which is not difficult to find.
If the value of the capsule and associated bridge capacitor is outside the useful range, one can encounter the dominant tuning peak where the inductor core slug is right up at one end of its range...... I've found it better to change oscillator frequency to bring the inductor slug position back within a more central location.... That seems to help with the system 'Q', and ultimately the noise figure.
There are a lot of variables within this simple circuit. I've not encountered anyone - so far - who has been able to rationalise the theoretical maths involved in the inductor assembly, so that we can work from a known 'status quo'.
It seems there are simply too many 'unknown variables', to allow 'sim' software to be very useful here, for example.
So practical experimentation seems to remain the best option at present.
This circuit
can work very well... but getting it to do so predictably is still a bit of a 'work in progress' !