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The effective acceleration of a body, when thrown upwards with acceleration aa (in a frame moving with acceleration aa) will be:

A

\sqrt{a - g^2}

B

\sqrt{a^2 + g^2}

C

(a - g)

D

(a + g)

Step-by-Step Solution

  1. Analyze the Frame of Reference: The problem describes a body being thrown upwards from a system (like a lift) that is accelerating with acceleration aa. The phrase 'thrown upwards with acceleration a' typically implies the frame of reference is accelerating upwards with aa.
  2. Effective Acceleration Concept: In a non-inertial frame of reference (accelerating frame), a pseudo-force acts on the body in the direction opposite to the frame's acceleration.
  • Acceleration of the frame = aa (upwards).
  • Acceleration due to gravity = gg (downwards).
  • Pseudo-acceleration acting on the body = aa (downwards, relative to the frame).
  1. Calculate Net Effective Acceleration: The effective acceleration (geffg_{eff}) experienced by the body is the vector sum of gravity and the pseudo-acceleration. geff=g+apseudo\vec{g}_{eff} = \vec{g} + \vec{a}_{pseudo} Since both act downwards: geff=g+ag_{eff} = g + a Therefore, the effective acceleration is (g+a)(g + a) or (a+g)(a + g) .
  2. Note on Answer Discrepancy: The 'Probable Answer' provided in the input is (ag)(a - g). This would be correct if the frame were accelerating downwards (where geff=gag_{eff} = g - a) or if aa referred to the net acceleration against gravity (anet=aappliedga_{net} = a_{applied} - g). However, for the standard case of 'upward acceleration', (a+g)(a + g) is the physically correct effective acceleration.
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