There's a book way to solve these problems, but there is a much better way if you don't care about any of the tensions...
Treat all 3 bodies as a system (as long as they all interact completely (no slack in ropes and no detachments pushing) and the ropes are massless), you need only consider forces that are external to the three blocks.
For the forces acting on the system we have F to the right and to the left we have m1μg + m2gμ + m3gμ
Static: Fmax = μs(m1+m2+m3)g So, FMax = (6kg)(9.8N/kg)(.6) = 35.28 N (anything F less won't budge anything)
Dynamic: F - μkmTg = mTa mT is the total mass (solve for a)
Now that you have a you can do a force balance around individual masses in order to find a Tension or interactive compressive force (like F12 , force of 1 on 2)
The net forces for m1, m2, m3 are m1a, m2a, m3a respectively.
The tension can be found by the net force on mass 3:
F-T-m3gμk = m3a (solve for T using the a which is the same for all the crates.
You should work out the force balances for m1 and m2 yourself. I will list them here for completeness. Note that textbooks usually want you to write these out, add them up (which results in the equation that I started with as all internal forces cancel for the system of 3 masses), and solve for a. You then solve for T and F12 the same way.
m2: F12 - m2gμk = m2a
m1: T - F21 - m1gμk = m1a
I'll leave you to answer the particular questions.