Rumplestiltskin said:
I'm baffled. They will meet at the same time, which is 16s. Therefore plugging this into the acceleration should give me the same distance of 192m. Otherwise the units do not work.
You are baffled because you don't write down the equations.
Using your terminology, we have:
for the car, driving at constant speed ##v=12\ m/s##: ##d_c(t)=vt##.
For the motorcyclist, driving from rest at constant acceleration ##a=1.5\ m/s²##: ##d_m(t)=\frac{1}{2}at²##.
As you are looking for the distance at which they meet, the equation to solve is ##d_c(t)=d_m(t)##.
You solved that part correctly, getting 16 seconds for ##t##.
Now all you have to do is plug in that value, 16, in the equation you have for ##d_c## or for ##d_m##. You are right, they both should give the same result, and they do.
Looking at dimensions is a good method to check whether a result makes sense. If you are computing a distance, and find a value in seconds, you know something went wrong.
But dimensions being correct is a necessary condition, not a sufficient one.
If a is an acceleration, and t a time, at² will be a value in meters. That is correct. But so will 10at², or 100at². All the products of at² with a dimensionless constant will give a value in meters. There is only one that gives you the distance traveled from rest when a is a constant acceleration: ##\frac{1}{2}at²##. The "pesky" ½ Ray mentioned.
That's why the exercise template contains a section "Relevant equations". Had you looked them up, written them down, and used them in the calculation, you would have solved this exercise in post 1.