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JEE PHYSICS MCQ: WORK-ENERGY-POWER

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A particle of mass 1 g1 \mathrm{~g} moving with a velocity u⃗1=(3i^−2j^)ms−1\vec{u}_1=(3 \hat{i}-2 \hat{j}) \mathrm{ms}^{-1} experiences a perfectly inelastic collision with another particle of mass 2 g2 \mathrm{~g} moving with a velocity u⃗2=(4j^−6k^)ms−1\vec{u}_2=(4 \hat{j}-6 \hat{k}) \mathrm{ms}^{-1}. The velocity (in ms−1\mathrm{m} \mathrm{s}^{-1}) of the combined particle is
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Correct option: A
i^+2j^−4k^\hat{i}+2 \hat{j}-4 \hat{k}
Option C (πa2μ0I2bωsin⁡ωt\frac{\pi a^2 \mu_0 I}{2 b} \omega \sin \omega t) is correct because it represents the induced emf in the smaller loop as a function of time, considering the changing magnetic flux due to rotation.

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