This is actually a really fun problem, as if you try to think through the rotational and linear acceleration in the normal frame of reference, the math gets complicated in a hurry. The last part should give us a hint that changing frame of reference will simplify things. In fact, if we consider everything from the frame of reference of the driver, the problem rapidly simplifies. From the driver's frame of reference, the door is experiencing an acceleration in the opposite direction of 2 ft/sec2. This then becomes a pendulum problem, although it is a rigid pendulum, not a simple pendulum. So, I = mL2/3. It starts with potential energy and no rotational kinetic energy. It ends (instant before slamming shut) with zero potential and all rotational kinetic energy. The potential energy lost is 1.25 ft * 2 ft/sec2 * m = 2.5m. So, if we set the kinetic energy at the bottom to this potential energy, we get
Iω2/2 = 2.5m
mL2ω2 / 6 = 2.5m
ω2 = 2.5*6/(2.5)2 = 2.4
ω = 1.55
Therefore, velocity of outside edge is angular velocity times radius or
1.55 * 2.5 = 3.875 ft/sec
1.55 * 2.5 = 3.875 ft/sec
If you have additional questions on that, please let me know.