The problem asks us to determine the time \( t \) when the acceleration of a particle becomes zero, given its position as a function of time: \( x = at^2 - bt^3 \).
\[ v = \frac{dx}{dt} = \frac{d}{dt}(at^2 - bt^3) = 2at - 3bt^2 \]
\[ a = \frac{dv}{dt} = \frac{d}{dt}(2at - 3bt^2) = 2a - 6bt \]
\[ 2a - 6bt = 0 \quad \Rightarrow \quad 2a = 6bt \quad \Rightarrow \quad t = \frac{2a}{6b} = \frac{a}{3b} \]
Hence, the time at which the acceleration of the particle becomes zero is \( \frac{a}{3b} \).