Read this:
http://injectordynamics.com/articles...racterization/
This is also interesting though not directly related
http://injectordynamics.com/articles...-and-dipshits/
Here is the formula for the slopes:
You can plot the slopes on wolfram alpha or a graphic package, change the breakpoint/offset/high/low slop and see how the curve changes.
IF (fuelmass >= breakpoint) y (fuelmass_lbs)*=**highslope_lb_sec * (x (injector_sec) - *(breakpoint* (1/lowslope_lb_s - 1/highslope_lb_s) + offset_sec))
IF (fuelmass <*breakpoint) y (fuelmass_lbs)*=**lowslope_lb_sec * (x (injector_sec) - *offset_sec)
fuelmass_lbs = airmass_lbs*/ commanded_AFR
Where offset is your injector offset (eg how long it takes for the injector to open and actually start flowing fuel)
Breakpoint is where the two slopes change, usually this is when the injector starts to flow linearly
Now the ecu actually feeds in desired*fuel mass and then gets injector ms, eg the opposite of how the equation looks. You can rearrange the formula if you wanted to do that.
Basically the whole point of the two slopes is to approximate the flow of a non linear injector. With the standard injectors this works pretty well, with large injectors it works not bad however you will have an error as can be seen in pauls graph of injector flow vs approximate flow. This isn't a huge deal but you can see why a nice lookup table would work better, problem is the ford ECU doesn't work that way.
edit: Increasing the high slope means a steeper graph, this means you will open the injector for less time for the same requested fuel mass. Bigger injectors flow more fuel, hence you want to open them less for a given air mass. Eg you want to lean the mixture out.