Re: The Carnot efficiency problem
Posted: Thu Aug 03, 2023 12:46 am
In my (simple) mind, it´s the pressure that´s doing the work, not the heat as so. The heat supply is causing the pressure to rise so you
can use it to preform mechanical work on a piston.
Then the pressure falls during the stroke from TDC to BDC and. When the pressure falls the temperature falls,
as known in the p*v/t = m*R/M equation.
And you are left with LESS heat. It is not "flown through" to the cold side.
It is easier (for me at least), to visualize the process as: Energy in form of heat, is converted to pressure, who is converted to mechanical work.
This way one can better understand why the heat had "disappeared" and not carried away in a cold sink.
It doesn't matter to me, if the process is isothermal or adiabatic, these are theoretical terms for ideal gasses/processes, who not occurs as so in praxis/nature.
The same is for the term Carnot efficiency. It´s only a theory who claims, that the efficiency of an engine ONLY depends on deltaT.
And (as Tom point´s out) that´s further more down to 0 Kelvin, regardless of what temperature you started with ? ? ?
If one would construct an engine only from these premise, you will end up with not trying anything practical, because in theory it´s a VERY bad idea. You will "loose" almost every Joule you have.
In theory, theory and praxis are the same. In praxis they are not . . .
I hope more people in this forum will do some practical experiments with their small Stirling engines. I should not be so difficult to
isolate the cold side of the engine and see if there is something to Tom´s experience.
- And you don´t need high precession thermocouple's to do this. Look for the tendencies, not the "correct" temperature.
But have anyone in here done that ?
Yes, I have my self ;-)
The Stirling cycle is a closed one. Everything are to be isolated from the environment . . .
And don´t just try to "push" more heat in to the engine, than it can convert to pressure and thereby work.
Think on, when water boils (in ambient pressure), you can´t raise the temperature in the water, no matter how much heat you are supplying.
can use it to preform mechanical work on a piston.
Then the pressure falls during the stroke from TDC to BDC and. When the pressure falls the temperature falls,
as known in the p*v/t = m*R/M equation.
And you are left with LESS heat. It is not "flown through" to the cold side.
It is easier (for me at least), to visualize the process as: Energy in form of heat, is converted to pressure, who is converted to mechanical work.
This way one can better understand why the heat had "disappeared" and not carried away in a cold sink.
It doesn't matter to me, if the process is isothermal or adiabatic, these are theoretical terms for ideal gasses/processes, who not occurs as so in praxis/nature.
The same is for the term Carnot efficiency. It´s only a theory who claims, that the efficiency of an engine ONLY depends on deltaT.
And (as Tom point´s out) that´s further more down to 0 Kelvin, regardless of what temperature you started with ? ? ?
If one would construct an engine only from these premise, you will end up with not trying anything practical, because in theory it´s a VERY bad idea. You will "loose" almost every Joule you have.
In theory, theory and praxis are the same. In praxis they are not . . .
I hope more people in this forum will do some practical experiments with their small Stirling engines. I should not be so difficult to
isolate the cold side of the engine and see if there is something to Tom´s experience.
- And you don´t need high precession thermocouple's to do this. Look for the tendencies, not the "correct" temperature.
But have anyone in here done that ?
Yes, I have my self ;-)
The Stirling cycle is a closed one. Everything are to be isolated from the environment . . .
And don´t just try to "push" more heat in to the engine, than it can convert to pressure and thereby work.
Think on, when water boils (in ambient pressure), you can´t raise the temperature in the water, no matter how much heat you are supplying.