Given mass \(m=20\) kg. Displacement \(x = 5t^2\) m.
Velocity \(v = \frac{dx}{dt} = \frac{d}{dt}(5t^2) = 10t \text{ m/s}\).
Acceleration \(a = \frac{dv}{dt} = \frac{d}{dt}(10t) = 10 \text{ m/s}^2\).
Force \(F = ma = 20 \text{ kg} \times 10 \text{ m/s}^2 = 200 \text{ N}\). (This force is constant).
Work done (W) can be calculated in two ways:
1. \(W = F \cdot s\) (if F is constant and along displacement s)
2. Work-Energy Theorem: \(W = \Delta K.E. = \frac{1}{2}m v_f^2 - \frac{1}{2}m v_i^2\).
Assuming the object starts from rest at \(t=0\), so \(v_i=0\). Then \(W = \frac{1}{2}m v_f^2\).
Work done in time \(t_1 = 3\) s:
Displacement at \(t_1=3\)s: \(x_1 = 5(3)^2 = 5 \times 9 = 45\) m.
Velocity at \(t_1=3\)s: \(v_1 = 10(3) = 30\) m/s.
Work done \(W_1 = \frac{1}{2}mv_1^2 = \frac{1}{2}(20)(30)^2 = 10 \times 900 = 9000\) J.
(Alternatively, \(W_1 = F \cdot x_1 = 200 \text{ N} \times 45 \text{ m} = 9000 \text{ J}\)).
Work done in time \(t_2 = 5\) s:
Displacement at \(t_2=5\)s: \(x_2 = 5(5)^2 = 5 \times 25 = 125\) m.
Velocity at \(t_2=5\)s: \(v_2 = 10(5) = 50\) m/s.
Work done \(W_2 = \frac{1}{2}mv_2^2 = \frac{1}{2}(20)(50)^2 = 10 \times 2500 = 25000\) J.
(Alternatively, \(W_2 = F \cdot x_2 = 200 \text{ N} \times 125 \text{ m} = 25000 \text{ J}\)).
The question asks for the ratio of work done "in times 3s and 5s". This usually means work done *up to* 3s and work done *up to* 5s.
Ratio \( \frac{W_1}{W_2} = \frac{9000 \text{ J}}{25000 \text{ J}} = \frac{9}{25} \).
This matches option (d).
If the question meant work done *during* the 3rd second and *during* the 5th second, the calculation would be different (Work done from t=2 to t=3, and t=4 to t=5). But "in times 3s and 5s" usually refers to the total work done from t=0 to t=3s and from t=0 to t=5s.
Since \(W \propto v^2\) and \(v \propto t\), then \(W \propto t^2\).
So, \(W_1/W_2 = (t_1/t_2)^2 = (3/5)^2 = 9/25\).
Also, \(W \propto x\) (since F is constant) and \(x \propto t^2\), so \(W \propto t^2\).
\[ \boxed{\frac{9}{25}} \]