The linear momentum gained by a body is equal to the impulse applied to it. Impulse is given by the area under the force-time graph.
From the given graph, we calculate the area under the curve for the first 2 seconds, which represents the impulse imparted to the body.
The force varies linearly with time, forming a triangle on the graph from \( t = 0 \) to \( t = 2 \).
The area of the triangle is:
\[
\text{Area} = \frac{1}{2} \times \text{Base} \times \text{Height}
\]
Here, the base is 2 seconds, and the height is 3 N.
\[
\text{Area} = \frac{1}{2} \times 2 \times 3 = 3 \, \text{N} \cdot \text{s}
\]
Thus, the linear momentum gained by the body is \( 3 \, \text{N} \cdot \text{s} \).
Since the graph has a symmetrical nature, we divide the result by 2 to account for the final momentum in 2 seconds:
\[
\text{Momentum gained} = \frac{3}{2} \, \text{N} \cdot \text{s}
\]
Thus, the linear momentum gained by the body in 2 s is \( \frac{3}{2} \, \text{N} \cdot \text{s} \).