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NEET PHYSICSMedium

A stone tied to a string of length LL is whirled in a vertical circle with the other end of the string at the centre. At a certain instant of time, the stone is at its lowest position and has a speed uu. The magnitude of the change in its velocity as it reaches a position where the string is horizontal is:

A

u22gL\sqrt{u^2-2gL}

B

2gL\sqrt{2gL}

C

u2gL\sqrt{u^2-gL}

D

2(u2gL)\sqrt{2(u^2-gL)}

Step-by-Step Solution

Let the initial velocity at the lowest point be vi=ui^\vec{v}_i = u \hat{i}. When the string is horizontal, the stone has reached a height LL . Let its velocity at this position be vf=vj^\vec{v}_f = v \hat{j}. Using the principle of conservation of mechanical energy: 12mu2=12mv2+mgL\frac{1}{2} m u^2 = \frac{1}{2} m v^2 + mgL v2=u22gLv^2 = u^2 - 2gL v=u22gLv = \sqrt{u^2 - 2gL} So, vf=u22gLj^\vec{v}_f = \sqrt{u^2 - 2gL} \hat{j}. The change in velocity is Δv=vfvi=u22gLj^ui^\Delta \vec{v} = \vec{v}_f - \vec{v}_i = \sqrt{u^2 - 2gL} \hat{j} - u \hat{i}. The magnitude of the change in velocity is: Δv=(u22gL)2+(u)2=u22gL+u2=2u22gL=2(u2gL)|\Delta \vec{v}| = \sqrt{(\sqrt{u^2 - 2gL})^2 + (-u)^2} = \sqrt{u^2 - 2gL + u^2} = \sqrt{2u^2 - 2gL} = \sqrt{2(u^2 - gL)}.

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