
- A$\frac{2}{3} R$
- B$\frac{1}{3} R$
- C$\frac{3}{5} R$
- ✓$\frac{4}{5} R$

$mR ^2 \omega=\left(m R^2 \times \frac{8 \omega}{9}\right)+\left(\frac{ m }{8} \times \frac{9 R^2}{25} \times \frac{8 \omega}{9}\right)+\left(\frac{ m }{8} \times x^2 \times \frac{8 \omega}{9}\right) \Rightarrow x=\frac{4 R}{5}$
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$S1:$ The efficiency of a heat engine can be $1,$ but the coefficient of performance of a refrigerator can never be infinity.
$S2:$ The first law of thermodynamics is basically the principle of conservation of energy.
$S3:$ The second law of thermodynamics does not allow several phenomena consistent with the first law.
$S4:$ A process,whose only result is to transfer heat from a colder to a hotter object, is impossible.

[specific heat of aluminium $= 0.91\,J/g\,\,^oc$ ]
