You’re getting there. Except that the original ghost ball line is adjusted slightly to make sure the ball does
get the ball to the ghost ball location.
The issue with squirt is a non-issue. From Dr. Dave research on squirt we have:
View attachment 528432
To give some context to the graph. The offsets were using parallel english. This means the torque line (the distance the cue line is from the center of mass when at 90°) is equal to the offset position. It’s basically the lever length that turns the ball on off center hits.
The measurements are in inches. So to compare deflection I will convert everything into mm, since tips use mm.
The largest offset is nearly 13mm. Remember the rounded ball surface and the tip shape determine the exact contact point as does the direction the cue is pointing. With a parallel cue line as used here, the contact point is likely near the inner edge of the shaft line.
The other offsets are 3.81 mm apart. The smallest offset graphed was .21", or 5.33mm. That offset on a hard hit deflected about 1°.
The proposed offset at the ball center was a dimes width or 1.35mm. If the testing has continued and the offset maintained the same incremental change, the next smallest test number would have been 1.5mm. Using the graphed results to establish a trend we find that each lesser offset reduced deflection around a single degree. Logic tells us that at a dimes width (1.35mm), the squirt is neglible, approaching zero. Dr. Dave concurred.
This test used a parallel cue line, the convergent cue line points back towards the center from the outside contact point,. This inflective line when input into the Ron Shepard deflection diagram finds the triangle created by the proposed offset to be a mere sliver. The cue line approaches the contact point to center of mass line, pj’s pet line.
I hope this helps you realize that squirt is not a real factor here. A similar analysis reveals that the same is true for throw, especially with convergent
inside english.