Ok, "we can also express the rate at which a force does work on a particle in terms of that force and the particle's velocity".
I'm trying to "see it" conceptually. My primary visualization is that I imagine an x-y coordinate system, x axis is displacement, y is force.
Now I "turn on" the x-axis like a treadmill, and set the treadmill to "5 meters per second" and the x-axis starts going left (i.e. 5 becomes 4, 4 becomes 3, etc...)
Now I "look" at the x-y coordinate system, and draw the Force function onto the graph as if the treadmill were switched off, between the limits of integration.
Now I sorta "visualize" what the result would be if I drew the graph while the X-axis was sliding (treadmill on) but I thought it was off (no sliding).
As a matter of fact, it would be a perfect "stretching" and the effect of the treadmill on the force*distance, is the effect of replacing displacement with velocity in the P=F*V equation! I think I got it!
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