Alright, I got it. One way of looking at it is in terms of internal energy. For an adiabatic expansion:
ΔU = -W = -PΔV
Then, using the ideal gas law:
-PΔV = nRΔT
Since it's an adiabatic expansion, W (and therefore, ΔU and PΔV) will be negative, which means nRΔT also has to be negative. Since n and R are both positive, then it means ΔT must be negative. The only way this can be true is if the initial temperature T1 is larger than the final temperature T2.