



To resolve this, we must examine the movement of a small steel sphere descending into a viscous medium such as glycerine.
Upon release, the steel sphere initially accelerates under gravity. However, as it penetrates the glycerine, it encounters an opposing viscous drag force, the magnitude of which escalates with its speed. Consequently, the sphere attains a constant speed, termed terminal velocity, at which point the resultant force acting upon it is null.
The forces influencing the sphere are:
These forces equilibrate, leading the sphere to achieve its terminal velocity \(v_t\).
The velocity-time graph for this phenomenon will exhibit:
The accurate graphical representation depicts an initial steep gradient that progressively flattens to a constant value, aligning with the accompanying image:
Therefore, the correct depiction is the option illustrated by the image, where velocity initially rises and subsequently stabilizes upon reaching terminal velocity.