Holmz said:
I am thinking that maybe there is a confusion on my part with the term "pressure wave".
Are you referring to a "wave of pressure" or "wave of flow which has pressure" and which is moving sub-sonic, or a pressure wave that is at the speed of sound?
In the
http://en.wikipedia.org/wiki/Cylinder_head_porting#Wave_dynamics" - It shows a graph, but looks like a modeled pressure, otherwise shouldn't there be higher frequency ripples from the vale opening and closing events?
Pressure wave at the speed of sound.
On the wikipedia link, you can see the blue line that is the pressure present at the back of the valve in the runner. The red line is the pressure measured at the runner's entrance.
Atmospheric pressure is 1 bar.
You can see that both measurements are going over and under atm pressure when the intake valve is closed (left side of the graph) and that they're out of phase.
The low pressure created by the downward motion of the piston sends a low pressure wave near the valve (blue line at around 435°), that pressure wave travels down the runner to arrive at around 500° at the runner's entrance (red line).
When that LOW pressure wave senses the large area change (runner's entrance-to-atmosphere, area change = \infty), it sends back a HIGH pressure wave that will traveled down the runner and that arrives at the valve at around 600° on the blue line.
Since at that point pressure in the cylinder (not shown on graph) is high and the valve is almost closed, it acts like a wall (area change = 0) and the pressure is "bouncing back", going again to the runner's entrance. In fact, the piston's upward motion contributes to the higher pressure wave sent back.
Once at the entrance, this high pressure wave is reflected as a low pressure wave. The whole process repeats itself until a high pressure wave arrives at the next intake valve opening, during valve overlap (the green area), which also helps filling the cylinder (at that point, the piston is going up, pushing the exhaust through the exhaust valve)
Once the piston is going down again, that destroys any residual pressure wave by creating a new strong one (back at the next 435°).
The phasing is determined by runner's length and RPM; Amplitude is determined by the runner's cross sectional area and the atmosphere's "cross sectional area" (which in this case is \infty). And for the case discussed in this thread, the atmosphere's "cross sectional area" would be replaced by the plenum's cross sectional area. If its size is too close to the runner's cross sectional area, the pressure wave will "see" that as a longer runner (runner's length + plenum's "length") which will screw up the phasing of the pressure wave pattern (The intake system will be tuned for a lower RPM).
Other interesting fact, high pressure wave travels faster than low pressure wave. You can see that with the orange lines and arrows on the graph. That is because the high pressure wave temperature is higher than the one for the low pressure wave, hence higher speed of sound. Furthermore, the speed of the pressure wave adds up with the speed of the air flow. So when going against the air flow, the speed of the pressure wave is reduced.
Although it would be weaker as the plenum gets bigger, but we did not cover the fact that the pressure wave that is reflected in the plenum will also come back to the runner ... and inside the other cylinder's runner too!
That is all based on 2-D calculations, throw in the third dimension and the fun begins.
This is why it is almost impossible to predict what is going to happen in an intake or exhaust system without accurate modeling and calculations. But understanding the principles will help us choose initial designs that may work.