Given the equation of motion:
\[
t = \alpha x^2 + \beta x
\]
To find the velocity \( \nu \), differentiate \( x \) with respect to \( t \):
\[
\frac{dx}{dt} = \frac{d}{dt} (\alpha x^2 + \beta x)
\]
Using the chain rule for \( x \) as a function of \( t \), we get:
\[
\frac{dx}{dt} = 2\alpha x \frac{dx}{dt} + \beta \frac{dx}{dt}
\]
This simplifies to:
\[
\nu = 2\alpha x + \beta
\]
Now differentiate \( \nu \) with respect to \( t \) to find the acceleration \( a \) (which is the derivative of velocity):
\[
a = \frac{d\nu}{dt} = 2\alpha \nu \frac{d\nu}{dt} + \beta \frac{d\nu}{dt}
\]
Thus, the retardation, which is the negative acceleration, is:
\[
\text{Retardation} = -a = - 2 \alpha \nu^3
\]