Franco, the concertina triode cathode idle voltage would indicate what idle and peak voltage difference occurs between that cathode and the valve's heater. For example, assuming 1mA through the concertina, the cathode idle voltage is about +70V, and the peak may get to about +140V. The heater is at nominal -12 to -24V, so the difference could be circa 100V idle and 160V peak, which is close or at limits depending on actual circuit voltages (and datasheet used). Swapping heater 1 and II provides a 12V margin to the datasheet limit.
If you changed to cathode bias then the total dc heater circuit could be isolated from 0V (assuming the filter caps can be isolated easily), and that heater circuit connected to an elevated DC voltage (even just connecting the negative end to 0V) so as to reduce any stress on the heater-cathode insulation, but note that the heaters are already effectively DC powered, so any benefit of elevation due to residual hum is likely down in the weeds anyway.
PS. In case you didn't notice, #1 tube heater gets a more filtered DC than #2 (due to an extra stage of RC ripple reduction), which is why they chose that original location, along with the grounded cathode input stage (and hence grid leak bias) for lowest hum from the very low microphone signal input.