Bruno's swirl can concept
Posted: Mon Apr 25, 2005 10:34 pm
SP-06 -- The Swirl Can Engine
Al, this is the first idea I would like to explore with you. It is extremely simple but needs an introduction so that the reasons behind it become clear. Namely, no one else appears to be thinking in the same direction, so the idea is obviously somewhat strange. I don’t know why – it looks perfectly logical to me. See if it appeals to you. Can you see something where I have gone wrong? Let me know what you think and we’ll talk.
I’ve been looking at pulsejets for perhaps 30 years. Some of their curious traits look like disadvantages to me and I have tried to find ways to remove them or wiggle out somehow if they cannot be removed.
One of the things I dislike is seemingly inherent in the pulsejet – the go-stop-go motion. First we use the partial vacuum to accelerate fresh air on its way into the chamber. Then we stop it dead. After that, we use combustion pressure to move it from standstill and accelerate it down the tailpipe.
To most people, this does not look like a big deal. After all, we are talking of a puff of air that needs to change speed or direction or both. Yet, to me, it has always looked wasteful. I mean, having that puff of gas move in the proper direction is what the jet engine is all about.
But, it took me a long time to come up with a way to avoid the stopping and the change of direction of gas in a pulsejet. The original inspiration came to me from Reynst, who avoided the loss of momentum in his pot combustor by having the mixture swirl in a toroidal vortex around an internal diffuser. I am fascinated by the Reynst concept, I must say. However, the Reynst pot is an unknown quantity, really. No one has seriously researched it but the guy himself. I wanted to see if the principle could be applied to something that was closer to the conventional pulsejet – but without increasing engine complexity.
Today, the answer looks simple and obvious to me, but it took me years to arrive at. I am just not a very quick thinker.
In the end, the trick was in changing the direction of incoming gases. In most conventional pulsejets, gases enter the combustion chamber in the direction of its longitudinal axis. In the Swirl Can, they enter perpendicular to the chamber and tangential to its section. Instead of the intake and exhaust being positioned at the top and bottom of a cylindrical can, I put them on the sides, tangential to the cylinder.
So, fresh air shoots in, follows the wall of the chamber and moves in a spiral motion, like the shape of the coil spring, towards the exhaust, slowing much less than it would if it shot out into the center of the can. It is not diffused because it is kept together between the can wall and the centrifugal force.
What will such motion accomplish? Well, I hope to induce the incoming mixture to generate a single big regular vortex rather than break out in myriad chaotic small ones. This vortex will act as a kind of flywheel, preserving the momentum of the charge.
If Reynst is right, such a vortex also acts a kind of a pump. It rotates away from the intake and thus sucks additional air in. This is helped by the fact that the intake protrudes some way into the chamber.
My bet is that the can will be refilled with a greater amount of mixture than with a conventional intake. This will make up for the fact that the charge is traveling at a greater speed than normal. At greater speed, its dynamic pressure is lower. We’ll have more charge at a somewhat lower pressure.
Keeping up the speed will delay ignition, further helping the swirl pump up the quantity of the mixture. This is considered a very good thing. The most efficient valveless pulsejets have very long induction periods. The French Escopette, for instance spends two thirds (!) of the entire cycle sucking mixture in. It is just about the most fuel-efficient pulsejet around.
True, some retained gas is coming into the chamber from the exhaust and moves in the opposite direction, but we are talking of low-density slow gas from the exhaust, which – I hope – will not be too effective in braking down the high-density fast gas from the intake.
It is generally thought that the ignition in a pulsejet is initiated by the mixing of the fresh charge with the free radicals remaining in the chamber and the tailpipe from the previous cycle. Reynst has shown that the tailpipe gas is not necessary. Both the ordinary jam-jars and the ‘serious’ Reynst pots get ignition without them, using just the free radicals in the boundary layer that clings to the chamber walls. Well, this should work here, too. Certainly the walls are going to be scrubbed quite thoroughly by the mixture swirling across them.
In conventional pulsejets, the incipient ignition that starts between the mixture and the free radicals is triggered into quick propagation throughout the mixture by two things. One is the hammer wave that accompanies the full refilling of the chamber (you can imagine it as the mixture front hitting the back wall of the chamber). The other is the pressure wave reflected from the end of the tailpipe. We have both here, just as in any other pulsejet. The difference is that in the Swirl Can, they will ‘slap’ the fresh charge from the side, rather than head on. This will not impede the circular motion, but will only increase the pre-combustion pressure. In a manner of speaking, the coiled spring will be compressed, but not unwound.
Combustion will take place within the swirl. Because combustion is chaotic and has no particular direction of its own, it will not fight against the direction of the swirl, either. My bet is that at worst, a great deal of the rotating momentum will be preserved right through the process. Indeed, Reynst says that combustion within a vortex adds speed to the spin. I don’t know enough about the vortices to be certain about it, but it sure sounds encouraging.
What keeps a vortex together is the balance of two forces. One is the centrifugal force that tries to break it apart and the other is the low pressure created in the center, which pulls it together. Combustion will produce additional gas and increase the internal pressure, so that this internal force pulling the vortex together will lessen. The centrifugal force will get the upper hand. This force and the rising pressure will both be forcing the exhaust gas out of the engine through the exhaust.
As the swirling combusting mixture reaches the exhaust – while its pressure is growing fast -- the direction of its motion will be right into the exhaust opening. Again, no change of direction – gas will just shoot off into the tailpipe on a tangent, as if released from a catapult, driven by both the gas pressure and the preserved momentum.
This is it, more or less. The intake is shown as a converging nozzle. This is the form it had on the drawing I used as the template – a paper on experiments with valveless pulsejets at the Department of Aerospace Engineering at the Indian Institute of Science, Bangalore, in 1998 and 1999. It may be a good thing, for it gives the incoming charge extra speed. However, it can also be a straight pipe or a diverging diffuser, for all I know. We can experiment with other shapes. I have no clear idea for the best location of the spark plug, but I don’t think it is very important.
Bruno
Hi Bruno,
Here are the sizes for the test:
Intake 5/8" ID X 3" L
Chamber 2 7/8" ID X 5" L
Exhaust 7/8" ID X 17" L
This compares to Sudarshan Kumar's as 1/5 area scale and 1/2 length scale, except for the intake which is 1/2.5 area and 1/3 length scale.
I used MAPP gas and a stinger for the initial test.
Some pops then a few " hoots " and then resonance.
With a few adjustments to fuel and air, and a warm system, the air and spark were shut off and the system sustained.
At low fuel rate, the sound is quite pleasant, and did not require ear protection. Near full throttle, the sound abruptly transitions to a snappy/snarly sound with no change in frequency but a definite increase in thrust ( but still not requiring ear protection ). At a slight increase in fuel flow beyond this point, the system abruptly quits.
Re starts are instantly accomplished ( when warm ) with spark, fuel, and a puff of air.
Your hand can be placed in the exhaust and intake flows within 8" with no discomfort; the intake having a greater apparent flow rate than the exhaust !
Notice the interesting heat pattern, opposite the intake, on the combustion chamber plating.
Al Belli
Al, this is the first idea I would like to explore with you. It is extremely simple but needs an introduction so that the reasons behind it become clear. Namely, no one else appears to be thinking in the same direction, so the idea is obviously somewhat strange. I don’t know why – it looks perfectly logical to me. See if it appeals to you. Can you see something where I have gone wrong? Let me know what you think and we’ll talk.
I’ve been looking at pulsejets for perhaps 30 years. Some of their curious traits look like disadvantages to me and I have tried to find ways to remove them or wiggle out somehow if they cannot be removed.
One of the things I dislike is seemingly inherent in the pulsejet – the go-stop-go motion. First we use the partial vacuum to accelerate fresh air on its way into the chamber. Then we stop it dead. After that, we use combustion pressure to move it from standstill and accelerate it down the tailpipe.
To most people, this does not look like a big deal. After all, we are talking of a puff of air that needs to change speed or direction or both. Yet, to me, it has always looked wasteful. I mean, having that puff of gas move in the proper direction is what the jet engine is all about.
But, it took me a long time to come up with a way to avoid the stopping and the change of direction of gas in a pulsejet. The original inspiration came to me from Reynst, who avoided the loss of momentum in his pot combustor by having the mixture swirl in a toroidal vortex around an internal diffuser. I am fascinated by the Reynst concept, I must say. However, the Reynst pot is an unknown quantity, really. No one has seriously researched it but the guy himself. I wanted to see if the principle could be applied to something that was closer to the conventional pulsejet – but without increasing engine complexity.
Today, the answer looks simple and obvious to me, but it took me years to arrive at. I am just not a very quick thinker.
In the end, the trick was in changing the direction of incoming gases. In most conventional pulsejets, gases enter the combustion chamber in the direction of its longitudinal axis. In the Swirl Can, they enter perpendicular to the chamber and tangential to its section. Instead of the intake and exhaust being positioned at the top and bottom of a cylindrical can, I put them on the sides, tangential to the cylinder.
So, fresh air shoots in, follows the wall of the chamber and moves in a spiral motion, like the shape of the coil spring, towards the exhaust, slowing much less than it would if it shot out into the center of the can. It is not diffused because it is kept together between the can wall and the centrifugal force.
What will such motion accomplish? Well, I hope to induce the incoming mixture to generate a single big regular vortex rather than break out in myriad chaotic small ones. This vortex will act as a kind of flywheel, preserving the momentum of the charge.
If Reynst is right, such a vortex also acts a kind of a pump. It rotates away from the intake and thus sucks additional air in. This is helped by the fact that the intake protrudes some way into the chamber.
My bet is that the can will be refilled with a greater amount of mixture than with a conventional intake. This will make up for the fact that the charge is traveling at a greater speed than normal. At greater speed, its dynamic pressure is lower. We’ll have more charge at a somewhat lower pressure.
Keeping up the speed will delay ignition, further helping the swirl pump up the quantity of the mixture. This is considered a very good thing. The most efficient valveless pulsejets have very long induction periods. The French Escopette, for instance spends two thirds (!) of the entire cycle sucking mixture in. It is just about the most fuel-efficient pulsejet around.
True, some retained gas is coming into the chamber from the exhaust and moves in the opposite direction, but we are talking of low-density slow gas from the exhaust, which – I hope – will not be too effective in braking down the high-density fast gas from the intake.
It is generally thought that the ignition in a pulsejet is initiated by the mixing of the fresh charge with the free radicals remaining in the chamber and the tailpipe from the previous cycle. Reynst has shown that the tailpipe gas is not necessary. Both the ordinary jam-jars and the ‘serious’ Reynst pots get ignition without them, using just the free radicals in the boundary layer that clings to the chamber walls. Well, this should work here, too. Certainly the walls are going to be scrubbed quite thoroughly by the mixture swirling across them.
In conventional pulsejets, the incipient ignition that starts between the mixture and the free radicals is triggered into quick propagation throughout the mixture by two things. One is the hammer wave that accompanies the full refilling of the chamber (you can imagine it as the mixture front hitting the back wall of the chamber). The other is the pressure wave reflected from the end of the tailpipe. We have both here, just as in any other pulsejet. The difference is that in the Swirl Can, they will ‘slap’ the fresh charge from the side, rather than head on. This will not impede the circular motion, but will only increase the pre-combustion pressure. In a manner of speaking, the coiled spring will be compressed, but not unwound.
Combustion will take place within the swirl. Because combustion is chaotic and has no particular direction of its own, it will not fight against the direction of the swirl, either. My bet is that at worst, a great deal of the rotating momentum will be preserved right through the process. Indeed, Reynst says that combustion within a vortex adds speed to the spin. I don’t know enough about the vortices to be certain about it, but it sure sounds encouraging.
What keeps a vortex together is the balance of two forces. One is the centrifugal force that tries to break it apart and the other is the low pressure created in the center, which pulls it together. Combustion will produce additional gas and increase the internal pressure, so that this internal force pulling the vortex together will lessen. The centrifugal force will get the upper hand. This force and the rising pressure will both be forcing the exhaust gas out of the engine through the exhaust.
As the swirling combusting mixture reaches the exhaust – while its pressure is growing fast -- the direction of its motion will be right into the exhaust opening. Again, no change of direction – gas will just shoot off into the tailpipe on a tangent, as if released from a catapult, driven by both the gas pressure and the preserved momentum.
This is it, more or less. The intake is shown as a converging nozzle. This is the form it had on the drawing I used as the template – a paper on experiments with valveless pulsejets at the Department of Aerospace Engineering at the Indian Institute of Science, Bangalore, in 1998 and 1999. It may be a good thing, for it gives the incoming charge extra speed. However, it can also be a straight pipe or a diverging diffuser, for all I know. We can experiment with other shapes. I have no clear idea for the best location of the spark plug, but I don’t think it is very important.
Bruno
Hi Bruno,
Here are the sizes for the test:
Intake 5/8" ID X 3" L
Chamber 2 7/8" ID X 5" L
Exhaust 7/8" ID X 17" L
This compares to Sudarshan Kumar's as 1/5 area scale and 1/2 length scale, except for the intake which is 1/2.5 area and 1/3 length scale.
I used MAPP gas and a stinger for the initial test.
Some pops then a few " hoots " and then resonance.
With a few adjustments to fuel and air, and a warm system, the air and spark were shut off and the system sustained.
At low fuel rate, the sound is quite pleasant, and did not require ear protection. Near full throttle, the sound abruptly transitions to a snappy/snarly sound with no change in frequency but a definite increase in thrust ( but still not requiring ear protection ). At a slight increase in fuel flow beyond this point, the system abruptly quits.
Re starts are instantly accomplished ( when warm ) with spark, fuel, and a puff of air.
Your hand can be placed in the exhaust and intake flows within 8" with no discomfort; the intake having a greater apparent flow rate than the exhaust !
Notice the interesting heat pattern, opposite the intake, on the combustion chamber plating.
Al Belli