Edub1 wrote:I thought about this but here is the problem.
The area of a circle is 3.14(r^2) right. This is not a linear equation, so increasing a .75" hole to 1" or so will yield only a fraction of the area increase that would be gained by increasing wheel size by .25"
Seeing as how the WG is not a restriction, this is not a good way to look at this.
Edub1 wrote:Also, you want to think in terms of pressure Vs momentum. You want to spin the turbo using the momentum of the exhaust gas as much as possible. Of course the resistance of the wheel creates back pressure and it is the combination of the two that spin the wheel.
Any momentum is largely attributed to flow and pressure differential across the turbo. While it is important to try and maximize momentum, it's effect is not going to be significant as flow and pressure differential.
Edub1 wrote:The WG, because of its physical properties, vents off only the excess pressure. I think it would be much better flow wise to try to minimize pressure as much as possible and capitalize on the force of the momentum of the flow.
For a given boost level (assuming same efficiencies), a better set-up is one that flows more air through a WG. Doing so generally means the turbo is using less air to spin the turbo. This is one way compressor and turbine efficiencies are important in making power.
Edub1 wrote:Say you need 80% to make boost and the stage 1 uses 40% flow + 60% backpressure. Then the WG bleeds off ~20% to hold boost steady. Here boost will hold using 40% flow and 40% backpressure
A stage 3 might use 70% flow and 30% pressure due to it's larger wheel area and of course empty space. Now our WG bleeds off the same 20%pressure and achieves the 80% needed to hold boost but 70% is force of flow (momentum) and 10% is backpressure.
In the first situation, venting more pressure will not work because it would only drop you out of boost faster because the smaller wheel uses backpressure and not force of flow to generate boost. Also, sufficiant quantities of gas can never escape through a WG untill their area has been sufficiantly reduced via backpressure. Think of adding an extra .5 " tailpipe to a 1" exhaust at a 90* angle - not gonna cut it.
Not sure exactly what you are trying to describe with the percentages. All turbos use the same physics to drive the turbine. All turbos use exhaust flow, heat, and pressure differential to drive it. Turbos can use varying amounts of each, but don't require a specific combination.
Edub1 wrote:Obviously the stage 1 is going to spool faster but the stage 3 wins in the high RPMs. At least that is how it works in my mind.
I think my super 60 with a stage 3 would be a great combo if I could find one cheep.
I appreciate the suggestion though - can you tell I thought about it a little bit?
The stage 3 would win in the high RPM's because it simply flows better and uses less exhaust energy to drive it in that RPM range. The motor sees less backpressure as a result freeing up some HP.
What you should consider is how the combinations of compressor and turbines work together. Matching their efficiency ranges to the same RPM's will yield the best results in terms of peak power over the range of RPM's where peak efficiencies occur. I'd suspect the Super 60 and Stage 3 turbine would be a decent match, but certainly not the best.
As far as your original post, it sounds like two things are going on. The choked feeling is simply not having enough turbo. A larger turbine may help, but stepping up to a T4 compressor would likely be a better solution. Compressor efficiency plays a large role in how hard the turbine has to work. Compressor efficiency is directly related to how aerodynamic the compressor is at a given flowrate and pressure ratio. IIRC, the Super 60 is dropping below 60 percent efficiency at redline at most boost levels on a KA. By contrast, a T04E 50 trim will still be in the 70's at redline. When the turbine needs to work less, more air will divert through the WG and consequently result in less backpressure on the motor. This results in more power at the crank.