Re: Tom is right, no heat sink req'd
Posted: Sat Jun 03, 2023 11:49 am
If you look at the standard "Carnot cycle" it consists of isothermal, followed by adiabatic expansion.
If you read Carnot's explanation in his book it reads:
But at that time Carnot had no concept whatsoever of heat being converted to "work".
Going on he wrote:
IMO rather than loosing heat during compression, while the gas is expanded and cold is when the working fluid has an opportunity to take in heat (on or near the hot side).
Maybe the heat is quantum tunneling out of the engine or some such thing, but the conventional explanations don't hold water IMO.
There is certainly SOME near isothermal transfer of heat when the engine is running at a very low speed, such as when starting up, or when under a heavy load perhaps, but as the RPM climbs, the ratio of adiabatic to isothermal, I should think, would tend more and more towards adiabatic.
The only time heat could be very quickly CONDUCTED out of the engine (from the working fluid) would be near TDC when the working fluid is compressed and very hot. When the ∆T is greater, then heat transfer is faster, but at that time, particularly in a thermal lag or thermal-acoustic type engine, all the working fluid is compressed and confined to the hot end. Likewise, though usually imperfect, in a Gamma, the displacer has working fluid, during compression, shifted over to the hot side, the cold side being covered/insulated from the working fluid by the displacer.
I don't see any real opportunity for "isothermal heat rejection". in an actual engine that is running up to operating speed.
If you read Carnot's explanation in his book it reads:
I can agree with this, but I also ask, why should it stop there? "Body B" is the "cold reservoir". The working fluid cools by expansion to become just as cold (if not colder).Thus rarefied, the temperature will fall spontaneously, as occurs with all elastic fluids; admit that the rarefaction may be continued to the point where the temperature becomes precisely that of the body B.
But at that time Carnot had no concept whatsoever of heat being converted to "work".
Going on he wrote:
This makes sense if we are talking about a slow isothermal process. As the gas is gradually compressed the heat that develops can be carried off, but in an engine turning at 3000 RPM, the gas already cold, (baring heat transfer to an equally cold "sink") you are talking compression at a rate much faster than a fire piston. The heat of compression doesn't have time to go anywhere. So the "heat out" during isothermal compression, I don't think can actually happen.(3) To condense the steam by putting it in contact with the body B, and at the same time exerting on it a constant pressure until it is entirely liquefied.
IMO rather than loosing heat during compression, while the gas is expanded and cold is when the working fluid has an opportunity to take in heat (on or near the hot side).
Maybe the heat is quantum tunneling out of the engine or some such thing, but the conventional explanations don't hold water IMO.
There is certainly SOME near isothermal transfer of heat when the engine is running at a very low speed, such as when starting up, or when under a heavy load perhaps, but as the RPM climbs, the ratio of adiabatic to isothermal, I should think, would tend more and more towards adiabatic.
The only time heat could be very quickly CONDUCTED out of the engine (from the working fluid) would be near TDC when the working fluid is compressed and very hot. When the ∆T is greater, then heat transfer is faster, but at that time, particularly in a thermal lag or thermal-acoustic type engine, all the working fluid is compressed and confined to the hot end. Likewise, though usually imperfect, in a Gamma, the displacer has working fluid, during compression, shifted over to the hot side, the cold side being covered/insulated from the working fluid by the displacer.
I don't see any real opportunity for "isothermal heat rejection". in an actual engine that is running up to operating speed.