Sorry guy, but I remember you never even being able to grasp the concept of a resonant radio signal....no surprise that you believe you won...I left the discussion with you out of sheer boredom...
You lost bad. Resonant radio signal is something you made up that has nothing to do with thermodynamics. Sheer boredom. That is so funny.
So you have a bad memory in addition to not being very bright. Here is a better explanation than I could give you although it is probably way over your head as well..

The
Cosmic Microwave Radiation (CMB) shows a blackbody spectrum of temperature 2.725 K
peaking at a wave length of about 0.2 cm beyond the far infrared spectrum. CMB is detected by radio-telescopes by resonance like radio antennas resonating with incoming radio waves thus generating a weak electrical signal which can be amplified into detection.
It would be difficult to detect CMB by thermal IR-imaging since the signal is very weak and thermal detection would require a detector at lower temperature than 2.725 K.
The concept of
Downwelling Longwave Radiation DLR from the cold atmosphere to the warm Earth surface plays a key role in CO2 alarmism. CMB is here presented as an ultimate form of DLR with the argument that a picture of CMB shows that DLR is real. If even the cold dark space is contributing to global warming, then global warming must be real, right?
Let us now scrutinize this argument in the setting of mathematical model of blackbody radiation studied in
Computational Blackbody Radiation, in the case of a radio-telescope as CMB-detector. The model takes the form of set oscillators with damping (see
here for some more details)
- Utt−Uxx−γUttt−h2Uxxt=f
where the subindices indicate differentiation with respect to space x and time t, and
- Utt−Uxx represents the oscillators in a wave model
- −γUttt is a dissipative term modeling outgoing radiation
- −h2Uxxt is a dissipative modeling internal heating
- f is incoming forcing/microwaves,
where γ represents the constant in Planck's radiation law and h represents a smallest mesh size, connected to dissipative losses as outgoing radiation and internal heating, respectively.
Microwaves are characterized by low frequency and long wave length (compared to visible and
infrared light) and in this case the dissipative loss of internal heating is small and is not detectable while the resonance can be detected after amplification just like a radio antenna is capable of detecting a weak radio wave by resonance followed by amplification.
Pictures of CMB are thus produced by an IR-camera in the form of a radio-telescope which works by resonance and not radiative heating. A CMB picture can therefore not be used as evidence that the weak glow of CMB acts as in a weak form of radiative heating named DLR or backradiation. This is because the CMB picture is not obtained from detection of radiative heating, but from resonance and amplification.
We conclude that a
CMB picture is not any evidence of DLR, because no DLR is detected.