The work done \( W \) by a force field \( \mathbf{F} \) in displacing a particle along a path \( \mathbf{r}(t) \) is given by the line integral:
\[ W = \int_C \mathbf{F} \cdot d\mathbf{r} \]
Where \( C \) is the curve along which the particle is displaced and \( \mathbf{r}(t) \) is the position vector of the particle along the curve. In this case, the curve is defined by:
Thus, the displacement vector is \( d\mathbf{r} = (dx, 0, dz) \), and the force field is \( \mathbf{F} = (2xy, 3x, -5z) \). We need to compute \( \mathbf{F} \cdot d\mathbf{r} \), which gives:
\[ \mathbf{F} \cdot d\mathbf{r} = (2xy, 3x, -5z) \cdot (2t, 0, 2t) = 4t(t^2 + 1)(t^2 + 1) - 5(t^2 + 1) \cdot 2t \]
Integrating this expression from \( t = 0 \) to \( t = 1 \), we get the work done:
\[ W = \int_0^1 \left( 4t(t^2 + 1)^2 - 10t(t^2 + 1) \right) dt \]
After performing the integration, we obtain:
\[ W = -\frac{21}{2} \]
The correct answer is option (C), \( -\frac{21}{2} \).