From the post "Neon Light Boom" dated 22 Dec 2017,
\(V_{min}=A\left(\cfrac{P}{T}\right)^2\)
where \(A=\cfrac{3.4354^2}{2}\cfrac{m_i^3}{qZ^2k^2}\)
if the basic particles involved are \(T^{-}\), then \(T\) decreases when \(V=V_{min}\) is applied. That in turn increases \(V_{min}\). Since \(v_{boom}\) is a resonance phenomenon, off \(v_{boom}\) values decrease its effect, \(T\) increases as \(V_{min}\) changes from \(V\). \(V_{min}\) decreases; we have an oscillation.
If an LED at \(280.73\,Hz\) (from the post "Freaking Out Entanglement" dated 14 dec 2017) is brighter, that it taps energy via entanglement, then this system made to oscillate at \(280.73\,Hz\) may just be supercooling.
It is possible to drive this system at \(280.73\,Hz\) irrespective of its natural resonance that depends on the the rate at which \(T^{-}\) is removed from the system. \(P\) increases with \(T\), but
\(PV=nRT\)
assures that the \(\cfrac{P}{V}\) is essentially a constant, given their inertia. \(A\) is a constant.
So, by regulating only the flow of \(T^{-}\) that controls \(T\), the system can be super cooling when it is oscillating at \(280.73\,Hz\). If the noble gas is made to circulate in a heat exchange, there is a certain velocity for a given set up (post "Heat Is The Predator" dated 7 Nov 2017) at which the system super cool. It does not matter the actual amplitude (\(\Delta T\)) of this oscillation as long as its frequency is at \(280.73\,Hz\).
Where do all the \(T^{-}\) particles come from? If the conduits are exposed, \(T^{-}\) particles are drawn from the the surroundings. But we think of this as cooling the conduit tubing as it heats up
when \(T^{-}\) particles are removed from it first. The removed \(T^{-}\) particles creates a temperature potential difference.
Such systems could already be in use in your refrigerators.
Note: \(280.73\,Hz\) is forced upon the system by changing \(T\) via the rate of flow of the inert gas in conduit pass a heat source.
The applied \(V\) is set at a nominal initial value when the system is prompted to oscillate. It too can be adjusted to achieve an oscillation frequency of \(280.73\,Hz\). In fact, \(V=V_{min}\) should be adjusted up as the system cools.
