A body is falling freely in a resistive medium. The motion of the body is described by \(\dfrac{dv}{dt}=(4-2v), \) where \(v\) is the velocity of the body at any instant (in \(\text{ms}^{–1}\)). The terminal velocity in this case refers to the velocity the body approaches as time \(t \to \infty.\) The initial acceleration and terminal velocity of the body, respectively, are:
1. |
\(4~\text{m/s}^2,\) \(2~\text{m/s}\) |
2. |
\(2~\text{m/s}^2,\) \(4~\text{m/s}\) |
3. |
\(6~\text{m/s}^2,\) \(2~\text{m/s}\) |
4. |
\(2~\text{m/s}^2,\) \(6~\text{m/s}\) |