To calculate the work done, we need to integrate the force over the displacement. Since the velocity is given as a function of \( x \), we can find the work done by using the work-energy theorem.
1. Step 1: Calculate the acceleration.
The velocity \( v \) is given by \( v = 2x^2 + 2 \). To find the force, we first need the acceleration, which is the derivative of velocity with respect to time. We use the chain rule:
\[
\frac{dv}{dt} = \frac{dv}{dx} \times \frac{dx}{dt} = a \times v
\]
First, calculate the derivative of velocity with respect to \( x \):
\[
\frac{dv}{dx} = 4x
\]
2. Step 2: Calculate the work done.
The work done is the integral of force over displacement. The force is \( F = ma = m \cdot \frac{dv}{dt} \). By substituting the values and integrating over the limits \( x = 0 \) to \( x = 2 \), we get:
\[
W = \int_{0}^{2} (2x^2 + 2) \, dx
\]
After performing the integration, we get the work done as:
\[
W = 6.4 \, \text{J}
\]
Thus, the work done is 6.4 J.