Second Sound of Radiotelegraphy static is Telekinesis from Helium to "Echo and or slang Piggyback"

Second sound is a quantum mechanical phenomenon in which heat transfer occurs by wave-like motion, rather than by the more usual mechanism of diffusion. Heat takes the place of pressure in normal sound waves. This leads to a very high thermal conductivity. It is known as "second sound" because the wave motion of heat is similar to the propagation ofsound in air.

Normal sound waves are fluctuations in the density of molecules in a substance; second sound waves are fluctuations in the density of particle-like thermal excitations (rotons and phonons^[1]). Second sound can be observed in any system in which most phonon-phonon collisions conserve momentum. This occurs in superfluids,^[2] and also in some dielectric crystals^[3][4][5] whenUmklapp scattering is small. (Umklapp phonon-phonon scattering exchanges momentum with the crystal lattice, so phonon momentum is not conserved.)

Second sound in helium II

Second sound is observed in liquid helium at temperatures below thelambda point, 2.1768 K, where ⁴He becomes a superfluid known as helium II. Helium II has the highest thermal conductivity of any known material (several hundred times higher thancopper).^[6] Second sound can be observed either as pulses or in a resonant cavity.^[7]

The speed of second sound is close to zero near the lambda point, increasing to approximately 20 m/s around 1.8 K,^[8]about ten times slower than normal sound waves.^[9] At temperatures below 1 K, the speed of second sound in helium II increases as the temperature decreases.^[10]

Second sound is also observed in superfluid helium-3 below its lambda point 2.5 mK.^[11]

Second sound in other media

Second sound has been observed in solid ⁴He and ³He,^[12][13] and in some dielectric solids such as Bi in the temperature range of 1.2 to 4.0 K with a velocity of (0.78±0.05)×10³ m/s,^[14] or NaF around 10 to 20 K.^[15]

Applications

Measuring the speed of second sound in ³He-⁴He mixtures can be used as athermometer in the range 0.01-0.7 K.^[16]

Oscillating Superleak Transducers (OST)^[17] use second sound to locate defects in superconducting accelerator cavities.^[18][19]