To solve the problem of finding the distance covered during the last $t$ seconds of ascent when a ball is thrown vertically upwards with speed $u$, we need to understand the physics involved in the motion under uniform acceleration due to gravity.
Concept: When the ball is thrown upwards, it will continue to ascend until its velocity becomes zero at the maximum height. The acceleration due to gravity $(g)$ acts downwards and affects the motion.
Now, consider the motion equations during the ascent:
Distance Calculated: To find the distance during the last $t$ seconds, we use the kinematic equation for distance: \( h = ut' - \frac{1}{2}g{t'}^2 \)
For the last $t$ seconds of the ascent, the initial velocity during these last seconds can be considered as \( v_o = g(t'-t) \) because: \( v_o = v + gt = 0 + g(t'-t) \)
The distance $d$ covered in the last $t$ seconds can be derived from: \( d = v_ot - \frac{1}{2}gt^2 \), where \( v_o = gt \).
Therefore, substituting \( v_o \) into the distance equation gives: \( d = gt\cdot t - \frac{1}{2}gt^2 = \frac{1}{2}gt^2 \)
Conclusion: Thus, the distance covered during the last $t$ seconds of its ascent is \(\frac{1}{2}gt^2\).