To find the acceleration of the particle as a function of its position \(x\), we start with the given velocity function:
v(x) = \beta x^{-2n}
where \(\beta\) and \(n\) are constants.
In kinematics, acceleration \(a\) is defined as the derivative of velocity \(v\) with respect to time \(t\). However, since velocity is given as a function of position, we can use the chain rule to find acceleration in terms of position:
a = \frac{dv}{dt} = \frac{dv}{dx} \cdot \frac{dx}{dt} = v \cdot \frac{dv}{dx}
First, calculate the derivative of \(v(x)\) with respect to \(x\):
\frac{dv}{dx} = \frac{d}{dx}(\beta x^{-2n}) = -2n\beta x^{-2n-1}
Since v(x) = \beta x^{-2n}, we substitute \(v\) and \(\frac{dv}{dx}\) into the expression for acceleration:
a = \left(\beta x^{-2n}\right) \left(-2n\beta x^{-2n-1}\right)
This simplifies to:
a = -2n\beta^2 x^{-2n} x^{-2n-1}
= -2n\beta^2 x^{-4n-1}
Therefore, the acceleration of the particle as a function of \(x\) is:
-2n\beta^2 x^{-4n-1}
This matches the given correct answer.