Stroller wrote: ↑Mon Apr 22, 2024 11:01 pm
Tom Booth wrote: ↑Sun Apr 14, 2024 7:18 am
Nobody could build a Carnot engine so how could you ever "prove" it isn't "the most efficient engine possible".
Well, after some thought, my reasoning was, If heat is, or isn't supposed to go through the engine and is or is not "converted" and all this is too difficult to trace or something, and you can't build a Carnot engine for comparison, we do at least have real engines and you should at least be able to catch the "rejected" heat leaving the engine on the "cold" side of a REAL engine and work backwards from there. How much heat does a Stirling engine actually "exhaust"?
The answer to this question is clearly "nearly all of it". That's why we get so few Watts of useful mechanical power out of our Stirling engines compared to the energy in the huge quantity of combusted gases we hurl at the hot side of the system.
And the heat isn't just leaving the cold side of the system. Everything radiates according to its temperature, in all directions. There's half your propane gone already. Its combustion heat never got transferred into the working fluid because it radiated back into the surrounding environment from the outside of the hot cap. That's your max efficiency down to 50%, regardless of whether Carnot is a dead dog or not.
Then ther'es the acoustic energy losses, or in less technical parlance, clanking...
I agree with the highlighted text.
I've said the same thing, and have asked if "rejection" in the Carnot limit applies to such heat that "never got transfered into the working fluid"..
For example, suppose an electric heating element is put inside the engine and the "hot side" is insulated with refractory, silica aerogel + vacuum, + infrared reflective gold lined whatever, so any heat escaping is negligible. Do we then include the waste heat from the coal burned at the electrical power plant? Or what is meant by "rejected" to the "cold reservoir".
Scientific terms should have well defined understandable terminology. What exactly "rejected" heat includes depends on who you ask.
Does it include heat that never entered the engine at all? If so, the "Carnot Limit" is meaningless, as that is a wild variable. In a solar heated Stirling, maybe that includes the entire heat output of the Sun, which, as you say: "radiates according to its temperature, in all directions".
Carnot, the presumed author of this arguably ambiguous terminology wrote pretty non-ambuguously:
The production of motive power is then due... not to an actual consumption of caloric, but to its transportation from a warm body to a cold body
And
According to established principles at the present time, we can compare with sufficient accuracy the motive power of heat to that of a waterfall. Each has a maximum that we cannot exceed, whatever may be, on the one hand, the machine which is acted upon by the water, and whatever, on the other hand, the substance acted upon by the heat. The motive power of a waterfall depends on its height and on the quantity of the liquid; the motive power of heat depends also on the quantity of caloric used, and on what may be termed, on what in fact we will call, the height of its fall, that is to say, the difference of temperature of the bodies between which the exchange of caloric is made. In the waterfall the motive power is exactly proportional to the difference of level between the higher and lower reservoirs. In the fall of caloric the motive power undoubtedly increases with the difference of temperature between the warm and the cold bodies; .
Later theoreticians seem to have dropped the "quantity" part, so the current "Carnot limit" equation has no "quantity" variable. Only Th and Tc. Nothing corresponding to Amps or "quantity of liquid" in a waterfall. Gallons per minute or anything else sensible
This is also fairly non-ambiguous:
In a Carnot heat engine, the heat expelled to a cold reservoir can be calculated using the formula Qc = Qh - W, where Qc is the heat expelled, Qh is the heat taken in from the hot reservoir, and W is the work output
That is the efficiency formula according to the first law, or the general conservation of energy. Not the Carnot limit formula
Q is an actual quantity of heat measured in joules, so also Qc and Qh. W= work, also measured in joules.
In any event, if you have a Stirling engine running on an ice cube, my question, or Tesla's related to how much heat passes through the engine to the ice?
Heat from a fire on the hot side radiating in all directions and never entering the engine so as to be transported through to the ice on the cold side is not involved, assuming the ice is otherwise perfectly insulated on all sides, other than where it is in direct contact with the cold side of the engine.
So,..
The debate, really, has long ago been narrowed down to the heat entering the engine and specifically the heat entering and expanding the working fluid. How much of THAT heat, that went into expanding the working fluid to produce work
MUST, according to the Carnot limit, pass through to the "ice" accelerating the melting rate?
Tesla suggested that because heat is energy and is converted into work by the heat engine rather than passing all the way through, a heat engine could, theoretically, run on the ambient heat of the atmosphere if maintained at a colder temperature on the opposite side, and that because the heat is transformed into "other forms of energy" after entering the engine, rather than passing all the way through to the cold, the "cold hole" could be maintained using less energy than would be gained from the conversion of the ambient heat.
In other words, you could have a kind of pseudo "perpetual motion", or a "Self-Acting engine", as it was called, by Carnot and Kelvin, who denied the possibility in their writings which Tesla had been reading.
In other words, Tesla thought he found a loophole in the 2nd Law of thermodynamics.
Arguably, we have working examples of Tesla's proposal:
https://youtu.be/caMuQbPwKYM?si=aumrc03uRkSykl3W
Evaporative cooling is driven by ambient heat. The toy bird is powered by ambient heat. You have a combined heat engine and ambient heat powered cooling system generating some electricity.
Some of the power generated is used to operate the cooling system; the bird wetting it's own head and swinging to accelerate evaporation, all within a "single heat reservoir". Arguably, something forbidden by some versions or interpretations of the second law of thermodynamics
A heat pump is really just a similar closed cycle evaporator. A fluid refrigerant evaporating in a closed cycle to produce cooling.
The suggestion however will immediately be pummeled and beaten about the head and ridiculed on the basis of the Carnot Limit. A supposed "universal law" that apparently forbids the existence of the drinking bird toy.
Personally I think that the drinking bird does exist. I used to play with one when I was maybe 4 years old, and watered it like a plant every day to keep its glass of water full
I've encountered at least one person on the science forums who said he does not believe that such a device as these drinking birds, or even a Stirling engine running on evaporative cooling could exist.
When I posted this video of a Stirling engine running on a wet piece of paper I was banned from the forum:
https://youtu.be/ARD3ctp80ac?si=0IlGAxiGZK4yXvDF
Another issue, of course, is there are various ways of measuring "efficiency". Thermal efficiency, mechanical efficiency, fuel burned vs. Power generated, "Carnot efficiency" etc