"Fast Combustion" vs. "Slow Combustion"&
Posted: Mon May 28, 2007 8:27 pm
In another thread Rmich732 kicked up perhaps the most contentious question in combustion guns.
1. Everyone agrees that there is an optimal C:B for a particular gun.
2. Usually the optimal C:B is somewhere in the range of say 0.7 ~ 1.0 for a basic combustion gun. Usually, folks assume that the number is actually 0.8. (Sometimes folks assume the number is 1.0 or 1.5.) It is assumed that changing things like the number of sparks or the fuel has an affect on the optimal C:B but the magnitude of these affect is not well understood.
3. For a particular chamber volume there is an optimal barrel volume (see points 1 and 2 above and Latke's data).
and the million dollar question....
4. For a particular barrel what is the optimum chamber volume? Is it the "Latke" C:B of 0.8?
We will define "optimal" and "maximum performance" as maximizing muzzle velocity, which is not the same as maximizing the efficiency of the gun.
If we make two guns with the same barrel;
a.) One of the guns has a chamber sized using the measured optimal C:B for the gun (for example you based the gun on Latke's)
b.) The other gun has a marginally larger chamber.
Which of these two guns will give higher muzzle velocities?
Assuming that by "marginally" larger we are talking about the C:B going from say 0.8 to 1.0. We are not talking about "mine" sized chambers or the C:B going to 10:1.
Bolingleadbath made an interesting point in Rmish's thread. There are perhaps two conflicting models of a basic combustion spud gun.
We will call the first model the "Fast Combustion" model. In the fast model combustion is complete (or is essentially complete) before the spud has moved significantly.
The second model is the "Slow Combustion" model. In this model, the spud starts to move long before combustion is complete.
(I tried to paraphrase BoilingLB, hopeful I'm pretty close to what he meant.)
These two models give very different predictions of the performance of a combustion gun.
One thing of interest is that in the fast model the combustion process is completely independent of the spud. The combustion process is essentially a "closed chamber" process.
In the slow model the combustion process (flame speed, pressure, burn time ...) responds to the movement of the spud.
The fast model would have many characteristics in common with a compressed air gun. In particular the pressure versus time curve would be qualitatively similar for the two types of guns. (Though the gas density is much lower in a combustion gun and heat loss affects a combustion gun much more than a compressed air gun.)
The slow model has little in common with a compressed air gun. In particular, there is no similarity between the pressure versus time curves of a combustion and a compressed gas gun.
The fast model predicts that an oversized chamber will increase performance. The fast model predicts that even a very large chamber will increase performance. ("Very large" is perhaps a C:B of 10:1)
The slow model predicts that ... not really sure what it predicts ... Depending on the details of the model and the details of what is really happening in the gun, and the characteristics of the gun, the slow model might predict a slightly larger chamber is better or it might predict that the optimal is the C:B predicted based on a variable barrel.
Anyone have any data for fast versus slow combustion?
I've got the "pressure" versus time data I recorded with a <a href="http://home.earthlink.net/~jimsluka/Pie ... tml">piezo and PC</a>. Clearly the P vs T curve is of a slow combustion process.
BoilingLB thinks Latke's data with multiple spark gaps supports the fast model. (Or the fast model is adequate to explain the experimental data.)
Any other thoughts?
Any thoughts, or better yet data, on the important question of a "reasonably" oversize chamber increasing performance for a particular barrel?
1. Everyone agrees that there is an optimal C:B for a particular gun.
2. Usually the optimal C:B is somewhere in the range of say 0.7 ~ 1.0 for a basic combustion gun. Usually, folks assume that the number is actually 0.8. (Sometimes folks assume the number is 1.0 or 1.5.) It is assumed that changing things like the number of sparks or the fuel has an affect on the optimal C:B but the magnitude of these affect is not well understood.
3. For a particular chamber volume there is an optimal barrel volume (see points 1 and 2 above and Latke's data).
and the million dollar question....
4. For a particular barrel what is the optimum chamber volume? Is it the "Latke" C:B of 0.8?
We will define "optimal" and "maximum performance" as maximizing muzzle velocity, which is not the same as maximizing the efficiency of the gun.
If we make two guns with the same barrel;
a.) One of the guns has a chamber sized using the measured optimal C:B for the gun (for example you based the gun on Latke's)
b.) The other gun has a marginally larger chamber.
Which of these two guns will give higher muzzle velocities?
Assuming that by "marginally" larger we are talking about the C:B going from say 0.8 to 1.0. We are not talking about "mine" sized chambers or the C:B going to 10:1.
Bolingleadbath made an interesting point in Rmish's thread. There are perhaps two conflicting models of a basic combustion spud gun.
We will call the first model the "Fast Combustion" model. In the fast model combustion is complete (or is essentially complete) before the spud has moved significantly.
The second model is the "Slow Combustion" model. In this model, the spud starts to move long before combustion is complete.
(I tried to paraphrase BoilingLB, hopeful I'm pretty close to what he meant.)
These two models give very different predictions of the performance of a combustion gun.
One thing of interest is that in the fast model the combustion process is completely independent of the spud. The combustion process is essentially a "closed chamber" process.
In the slow model the combustion process (flame speed, pressure, burn time ...) responds to the movement of the spud.
The fast model would have many characteristics in common with a compressed air gun. In particular the pressure versus time curve would be qualitatively similar for the two types of guns. (Though the gas density is much lower in a combustion gun and heat loss affects a combustion gun much more than a compressed air gun.)
The slow model has little in common with a compressed air gun. In particular, there is no similarity between the pressure versus time curves of a combustion and a compressed gas gun.
The fast model predicts that an oversized chamber will increase performance. The fast model predicts that even a very large chamber will increase performance. ("Very large" is perhaps a C:B of 10:1)
The slow model predicts that ... not really sure what it predicts ... Depending on the details of the model and the details of what is really happening in the gun, and the characteristics of the gun, the slow model might predict a slightly larger chamber is better or it might predict that the optimal is the C:B predicted based on a variable barrel.
Anyone have any data for fast versus slow combustion?
I've got the "pressure" versus time data I recorded with a <a href="http://home.earthlink.net/~jimsluka/Pie ... tml">piezo and PC</a>. Clearly the P vs T curve is of a slow combustion process.
BoilingLB thinks Latke's data with multiple spark gaps supports the fast model. (Or the fast model is adequate to explain the experimental data.)
Any other thoughts?
Any thoughts, or better yet data, on the important question of a "reasonably" oversize chamber increasing performance for a particular barrel?