Net work = change in kinetic energy:
$$W_\text{net} = \Delta K = K_f - K_i = \frac{1}{2} m (v_f^2 - v_i^2)$$
$$v_i = a (0)^{3/2} = 0 \, \text{m/s}$$
$$v_f = 5 \times (2)^{3/2} = 5 \times (2\sqrt{2}) = 5 \times 2.828 = 14.14 \, \text{m/s}$$
$$v_f^2 = (14.14)^2 = 200 \, \text{m}^2\text{/s}^2$$
$$W_\text{net} = \frac{1}{2} \times 0.5 \times (200 - 0) = 0.25 \times 200 = 50 \, \text{J}$$
\(W = \textbf{50 J}\)
Acceleration: \(a_x = \frac{dv}{dt} = v \frac{dv}{dx}\)
$$v = 5 x^{3/2}, \quad \frac{dv}{dx} = \frac{15}{2} x^{1/2}$$ $$F = m v \frac{dv}{dx} = 0.5 \times 5 x^{3/2} \times \frac{15}{2} x^{1/2} = \frac{75}{4} x^2$$
$$W = \int_0^2 F \, dx = \frac{75}{4} \int_0^2 x^2 \, dx = \frac{75}{4} \times \frac{8}{3} = 50 \, \text{J} \quad \checkmark$$
Work-energy theorem simplifies variable force problems. Direct \(\Delta KE\) always works!