Rarefication
Posted: Mon Aug 31, 2020 3:06 am
In my general quest to understand what makes a Stirling engine tick, and in particular, how can it (sometimes) run, without any need for a flywheel, I spent some time watching this video.
https://youtu.be/_5fv-xFuozs
As can be seen, when heat is first applied, (around 2:00) the piston immediately moves outward to the furthest existent possible with the expansion of the heated air.
With every subsequent attempt to get the engine going, the piston returns to this position, indicating, to me, anyway, that the air in the cylinder is still taking in heat and expanding, pushing the piston outward to the farthest limit.
After a certain time, however, some change takes place, and the engine begins to rock back and forth "on its own".
At this point, the piston is not only pushed out by the expanding gas, but is also in some way pushed or drawn back in.
This "drawing in" increases more and more, the direction of the flywheel actually reversing, so that, it would seem to me, at least, that not only is the piston NOT helping to push the piston in, but this "drawing inward" takes place, even in direct opposition to the inertia of the flywheel.
At some point, the rocking back and forth builds up to a point where the engine gats over the "hump" and takes off. From there it gradually picks up speed.
So what is going on?
Why the sudden change.from only pushing the piston outward to its furthest extent to eventually pulling or drawing the piston back inward?
My tentative speculation by logical deduction at this point goes something like this.
Of course, the engine has to reach "operating temperature", but what is so special about some specific operating temperature?
As the engine heats up more and more, the air inside expands more and more, gets hotter and hotter.
Logically, the gas, having nowhere to go LEAKS OUT, around the piston.
So, as time goes by, the air in the engine gets thinner and thinner, or more and more rarefied, as it gets hotter and hotter and more and more leaks out.
At some point, the gas becomes so uniformly hot and "thin" or rarefied that the few molecules left, are moving fast, striking the piston with much force and transferring a high proportion of their kinetic energy with each cycle.
A certain degree of rarefication has been reached where the heat added each cycle is balanced by the heat converted (kinetic energy transfered to the piston/flywheel/load).
Why should this rarefication be necessary?
Because otherwise there are too many hot molecules pushing out, all crowded together, bumping into each other, but not hot or fast enough to all impact and transfer energy to the piston.
Remember that, for a transfer of energy to take place, the piston has to be able to MOVE. It is the "give" of the piston that allows it to take in kinetic energy. The walls of the cylinder do not move, do not "give" so the speedy, fast, freely moving molecules mostly just bounce off the walls of the cylinder and do not give up their kinetic energy until they happen to strike the piston, which does give or move, so a transfer or conversion of energy takes place.
The "thinner" the air, the more freely the molecules can move and the more likely nearly all of them, moving at nearly the speed of light, will have a chance to strike the piston in a given cycle, so the more thorough is the energy transfer, and therefore, the more pronounced becomes the adiabatic cooling of the gas, the conversion of heat into mechanical movement, which results in the "weakening" of the molecules, or cooling, or lack of kinetic energy, which then gives the more dense, relatively MORE energetic outside atmospheric air molecules a chance to push the piston back inward, the very few internal air molecules having become suddenly weakened from impacting the piston and giving up their energy to it.
So, my conclusion is, then, for a Stirling engine to be able to run efficiently, and especially, to be able to do so without a flywheel, the gas inside the engine has to be sufficiently rarefied so that adiabatic cooling can be most effective.
Without the freedom to move, the molecules are too crowded, too sluggish, too dense, so that they spend more time bumping into each other than they do impacting the piston.
Perhaps this is why a very rarefied gas, like helium, gives a Stirling engine such a boost, even at relatively low temperatures, because the gas is already rarefied. Helium has such a very low boiling point that even ambient heat is extremely hot to it, so helium is very light and thin at ambient temperature.
https://youtu.be/Tlwu2UUIImo
https://youtu.be/_5fv-xFuozs
As can be seen, when heat is first applied, (around 2:00) the piston immediately moves outward to the furthest existent possible with the expansion of the heated air.
With every subsequent attempt to get the engine going, the piston returns to this position, indicating, to me, anyway, that the air in the cylinder is still taking in heat and expanding, pushing the piston outward to the farthest limit.
After a certain time, however, some change takes place, and the engine begins to rock back and forth "on its own".
At this point, the piston is not only pushed out by the expanding gas, but is also in some way pushed or drawn back in.
This "drawing in" increases more and more, the direction of the flywheel actually reversing, so that, it would seem to me, at least, that not only is the piston NOT helping to push the piston in, but this "drawing inward" takes place, even in direct opposition to the inertia of the flywheel.
At some point, the rocking back and forth builds up to a point where the engine gats over the "hump" and takes off. From there it gradually picks up speed.
So what is going on?
Why the sudden change.from only pushing the piston outward to its furthest extent to eventually pulling or drawing the piston back inward?
My tentative speculation by logical deduction at this point goes something like this.
Of course, the engine has to reach "operating temperature", but what is so special about some specific operating temperature?
As the engine heats up more and more, the air inside expands more and more, gets hotter and hotter.
Logically, the gas, having nowhere to go LEAKS OUT, around the piston.
So, as time goes by, the air in the engine gets thinner and thinner, or more and more rarefied, as it gets hotter and hotter and more and more leaks out.
At some point, the gas becomes so uniformly hot and "thin" or rarefied that the few molecules left, are moving fast, striking the piston with much force and transferring a high proportion of their kinetic energy with each cycle.
A certain degree of rarefication has been reached where the heat added each cycle is balanced by the heat converted (kinetic energy transfered to the piston/flywheel/load).
Why should this rarefication be necessary?
Because otherwise there are too many hot molecules pushing out, all crowded together, bumping into each other, but not hot or fast enough to all impact and transfer energy to the piston.
Remember that, for a transfer of energy to take place, the piston has to be able to MOVE. It is the "give" of the piston that allows it to take in kinetic energy. The walls of the cylinder do not move, do not "give" so the speedy, fast, freely moving molecules mostly just bounce off the walls of the cylinder and do not give up their kinetic energy until they happen to strike the piston, which does give or move, so a transfer or conversion of energy takes place.
The "thinner" the air, the more freely the molecules can move and the more likely nearly all of them, moving at nearly the speed of light, will have a chance to strike the piston in a given cycle, so the more thorough is the energy transfer, and therefore, the more pronounced becomes the adiabatic cooling of the gas, the conversion of heat into mechanical movement, which results in the "weakening" of the molecules, or cooling, or lack of kinetic energy, which then gives the more dense, relatively MORE energetic outside atmospheric air molecules a chance to push the piston back inward, the very few internal air molecules having become suddenly weakened from impacting the piston and giving up their energy to it.
So, my conclusion is, then, for a Stirling engine to be able to run efficiently, and especially, to be able to do so without a flywheel, the gas inside the engine has to be sufficiently rarefied so that adiabatic cooling can be most effective.
Without the freedom to move, the molecules are too crowded, too sluggish, too dense, so that they spend more time bumping into each other than they do impacting the piston.
Perhaps this is why a very rarefied gas, like helium, gives a Stirling engine such a boost, even at relatively low temperatures, because the gas is already rarefied. Helium has such a very low boiling point that even ambient heat is extremely hot to it, so helium is very light and thin at ambient temperature.
https://youtu.be/Tlwu2UUIImo