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If a ball is thrown vertically upwards with speed uu, the distance covered during the last tt seconds of its ascent is

A

12gt2\frac{1}{2}gt^2

B

ut12gt2ut - \frac{1}{2}gt^2

C

(ugt)t(u-gt)t

D

utut

Step-by-Step Solution

  1. Symmetry of Motion: In the absence of air resistance, time symmetry exists for projectile motion under gravity. The distance covered by an object during the last tt seconds of its upward journey is equal to the distance covered by a freely falling object during the first tt seconds of its downward journey from the maximum height .
  2. Free Fall Condition: At the maximum height, the final velocity of the ascent becomes zero, which acts as the initial velocity (u=0u' = 0) for the descent (free fall).
  3. Calculation: Using the second equation of motion for the downward journey: h=ut+12gt2h = u't + \frac{1}{2}gt^2 Substituting u=0u' = 0: h=0(t)+12gt2h = 0(t) + \frac{1}{2}gt^2 h=12gt2h = \frac{1}{2}gt^2.
  4. Alternative Method: At time (Tt)(T-t), where T=u/gT = u/g is the total time of ascent, the velocity is v=ug(Tt)=ug(u/gt)=gtv = u - g(T-t) = u - g(u/g - t) = gt. The distance covered in the remaining time tt with initial velocity gtgt and retardation g-g is s=(gt)t12gt2=12gt2s = (gt)t - \frac{1}{2}gt^2 = \frac{1}{2}gt^2.
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