Thermolelctric
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I must admit that there was logical mistake in my COP=5 cycle. The heat pump will not pump any more when the cold reservoir is heated(above the ambient) back from hot reservoir. Thanks everybody for explaining patiently.
So there is no other limitation to the COP than COP≤Th/(Th−Tc).
The COP can be very high if temperature dT is very small.
The practical heat pumps COP is so much below the theoretical maximum only because the various constructional problems.
The other interesting question is: theoretically, can we run the heat engine outside the building and use the work from the heat engine to run the heat pump to heat the building from the outside air and get the same amount or more heat, than burning the fuel inside the building with 100% efficiency?
So there is no other limitation to the COP than COP≤Th/(Th−Tc).
The COP can be very high if temperature dT is very small.
The practical heat pumps COP is so much below the theoretical maximum only because the various constructional problems.
The other interesting question is: theoretically, can we run the heat engine outside the building and use the work from the heat engine to run the heat pump to heat the building from the outside air and get the same amount or more heat, than burning the fuel inside the building with 100% efficiency?