Solution:
Given acceleration:
\[
a = \alpha t + \beta
\]
The velocity after time \(t\) is:
\[
v(t) = \frac{\alpha t^2}{2} + \beta t
\]
Given acceleration:
\[
a = \alpha t + \beta
\]
The velocity after time \(t\) is:
\[
v(t) = \frac{\alpha t^2}{2} + \beta t
\]
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