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The
classic contruction of a Stirling engine
The air in a Stirling engine is cyclically displaced in a closed volume
from a hot to a cold zone. As a result this air expands and shrinks
also cyclically, providing the aternating force on the working piston;
see the page about the Working
principle of a Stirling engine.
In the classic
construction the air displacer is a piston that moves in a so called
"hot cylinder" with some space, so that the air can pass between
this displacer and the internal cylinderwall. The displacer and the
working piston are both connected to a crankshaft with a flywheel on
it.
This altenative Stirling
design.
In this design the displacing of
the air is realized in a complete different way. Three ceramic solid
balls can roll in a glass test tube that is heated at the closed end
of it with a spirits burner. This rolling balls displace the air in
the tube from the hot zone to the cold zone and vice versa.
I found this "ball concept" on an internet website, where
it was implemented in a test tube Stirling, mend for education purposes.
The test tube with solid glass balls in it was connected to a separate
cylinder with the working piston by means of a flexible rubber tube.
Earlier I build two somewhat more sophisticated versions of this concept
which I named "Stirling Onrust"; see the models "Stirling
Onrust Jan" and "Stirling
Onrust Maarten". "Onrust" is dutch for"restless"
and this is more or less the character of these models. Nice Stirlings
if you ask me, but a little bit instable, despite the implementation
of a pendulum as a stabilization element.
To realize a more controlled running variant I presumed that I had to
eliminate the rubber tube and implement a flywheel in stead of a pendulum.
The only question was if a flywheel could keep an implicit equilibrium
in
score in this moving
system because a flywheel is a constant and a not re-adjustable element.
But it appears that the luck was with the fool again.
In this new and very unique design the working cylinder with piston
is directly and gastight connected to the open cold end of the glass
tube. This assembly of glass tube (as "hot cylinder") and
the cylinder with the working piston can swing in
the vertical plane around
a horizontal axis. The push rod of the working piston is connected to
a singular crankshaft with the flywheel on it. I
use ceramic solid balls because almost all glass balls easely burst
when they are heated.
This construction fulfill implicitly the demanding condition for each
Stirling that the ball displacer and the working piston are under 90º
in the moving diagram.
The motion of this engine is very sereen with a constant low tempo of
about 40 strokes per minute. It does think of an oilpump in the field
which is called a "Ja Knikker" in dutch; free translated:
a "yes-nodder". And this is the reason why I gave this Stirling
this name.
The flywheel doesn't run in the usual way with a relative high and constant
revolution speed. It is curious to see how the flywheel is pushed two
times in the cycle, due to the expanding and the shrinking of the air
in the system and how it helps the motion to get over the two dead points
in the cycle. In my opinion this model is one of the most "basic"
and tranparant designs of a Stirling engine.
A remarkable teamwork of divergent phenomena !
For those who want to see it here an almost perfect teamwork
between a number of different mechanical and physical phenomena executes
itself:
1.
The crankshaft not only transposes the alternating piston motion into
a rotating motion of the flywheel, but it also causes the swinging of
the assembly glass tube/working cylinder. This in combination with the
special attachment of the cylinder in a fork;
2. It is the gravitation force that causes the ceramic balls rolling
from left to right and vice versa;
3. The rolling balls pushes the air in the glass tube from the hot to
the cold zone and reverse;
4. Due to this displacement the captured air expands and shrinks by
which the working piston encouters a force two times in the cycle that
reverses on the right moment in that cycle;
5. The flywheel helps the motion to get over the two dead points in
the cycle, so that that the motion is repeating as long as the spirits
burner supplies energy to the system;
6. Is is
mainly the mass-inertness of the balls that determines the very sereen
and constant tempo of the oscillating motion of the engine.
A physically
orientated spectator may say that this is all obvious. But in my modest
opinion it is very wondrous that this harmonious teamwork between so
divergent phenomena takes place in such an uncomplicated engine design
!
Ceramic balls
For most modelbuilders it will be difficult to obtain ceramic balls. I could obtain some from my former employer where they are used to pulverize powders in a mill.
It is possible to use play marbles but most glass marbles have such high thermal tension that they burst easily if heated. But apparently there are such marbles with low thermal tension that survive the heat, but you can see that on the outside; it is a matter of luck then.
Ceramic marbles with (by accident) the right diameter (about 13mm) can be bought for reasonable low price; see:
http://www.freie-waffen.com/catalog/72keramikkugelnfrsteinschleuder-p-754.html
Some specifications
Outlines l*w*h=
170*100*120mm;
Diameter working piston= 11mm, the stroke= 11mm;
Diameter glass test tube= 15,5 * 14,2mm, the length= 75mm;
Diameter ceramic balls= about 13mm;
Diameter brass flywheel= 65mm, width= 10mm.