Techlib has many interesting lightting detection tips

However, around 300kHz RF receivers are used too.
For example in this "Basic low-power receiver" 330uH & 680pF LC resonant frequency is about: 340 kHz

I'm not sure why not to use for example: 20uH & 10 nF which gives about 350 kHz but we have 10 times smaller inductor?
Is it something with Q factor of this LC circuit, but while there is no pararell resistor R, so while this Q factor in RLC circuit is given by equation:
Qrlc(f,L,R):= (2*pi*f*L)/R;
can I assume that R goes to infinity and Q factor to 0?
It looks like that 10mH choke is antena support to help receive LF RF and to get similar resonant frequency in LC series circuit this tiny capacitor mentioned below should have value around 22pF when 10mH choke is used-we get then around 340kHz

These radio "crackles" are picked up by the antenna with the help of the 10 millihenry choke. Short antennas (short compared to the wavelength, that is) behave as though a very tiny capacitor is connected in series and this choke resonates with this capacitor allowing current to flow into the receiver.
While I'd like connect AM radio demodulated output from this basic receiver to ADC small MCU AVR pin and try to make post processing of these crack lighting strikes noise and make decision in software to qualify it to lighting strike or not depending on feedback from sound & light detection sensors too, maybe opamp amplifier with gain I do not know 50-100 could be better than this simple transistors based?
I think I need for the moment understand better this Q factor influence on received signal in LC/RLC circuits while one can get the same resonant frequency
1/(2*3.1415*sqrt(L*C)) [Hz]
using smalller inductor & bigger capacitor and reverse.
Are there any issues when I use 22uH & 10nF (LC) in schematics above to get around 340kHz resonant frequency?
Maybe there are tolerance issues of this LC components, but I do not need tune to exactly to 340kHz in this project I guess.
Update: According to
http://en.wikipedia.org/wiki/RLC_circuit#Q_factor The Q factor is a widespread measure used to characterise resonators. It is defined as the peak energy stored in the circuit divided by the average energy dissipated in it per radian at resonance. Low Q circuits are therefore damped and lossy and high Q circuits are underdamped. Q is related to bandwidth; low Q circuits are wide band and high Q circuits are narrow band. In fact, it happens that Q is the inverse of fractional bandwidth
Maybe it could be good idea add pararell resistor to this 340kHz LC, but while I do not need narrow band, which Q factor choose?
For example with 22uH inductance and 100k resistor I have Q factor:
Qrlc(340*kHz,20*uH,100*1000)= 0.00047
when 330uH is used I have 15 times bigger

Qrlc(340*kHz,330*uH,100*1000)= 0.00705