MCQ
A man slides down a light rope whose breaking strength is $\eta$ times the weight of man $(\eta<1)$. The maximum acceleration of the man so that the rope just breaks is ........
- ✓$g(1-\eta)$
- B$g(1+\eta)$
- C$g n$
- D$\frac{g}{\eta}$
Given that $T_{\max }=\eta w$
Using $F_{\text {net }}=m a$
$w-T_{\max }=\frac{w}{g} a$
$T_{\max }=\eta w$
So $a=g(1-\eta)$
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$T_{1}=27^{\circ} C$ [outside fridge]
$T_{2}=-23^{\circ} C$ [inside fridge]