vboom=3.4354∗densityZ
f=vλ
and for a torus with a noble gas collector channel of radius r,
2πr=λ
To be around the torus at f=280.73Hz,
r=vboom2πf=3.43542πf∗densityZ
It is possible for r→nr, a bigger torus that will accommodate n wave around the channel. To induce n standing wavelength in the channel, 2∗n equally spaced points along the circular channel will have to be shorted to ground, using conductors that draw T− particles.