Given that the acceleration is constant, we start with:
\(v = u + at\)
When the velocity has increased by \(50\, m/s\), the equation becomes:
\(u + 50 = u + a \)
\(a = 50\, m/s^2\)
To find the distance traveled by the particle in (t + 2)th second, we use:
\(S_n = u + \frac{a}{2}[2n-1]\)
For n = t + 2 (i.e., the (t + 2)th second):
\(S_{t + 2} = u + \frac{50}{2}[2(t + 2) - 1]\)
\(S_{t + 2} = u + \frac{50}{2}[2(t + 2) - 1]\)
\(= u + 25 \times [2(t + 2)- 1]\)
\(= u + 25(2t + 4 - 1)\)
\(= u + 25 (2t +3)\)
\(= u + 50t + 75\)
\(= 100 + 75\)
\(= 175\, m\)