(d) Here, the constant horizontal force required to take the body from position 1 to position 2 can be calculated by using work energy theorem. Let us assume that body taken slowly so that its speed doesn’t change, then $\mathrm{\Delta}K = 0$
$= W_{F} + W_{Mg} + W_{tension}$
(symbols have their usual meanings )
$W_{F} = F \times l\sin{45{^\circ}},$
$W_{Mg} = Mg(l - l\cos{45{^\circ}),W_{tension} = 0}$
$\therefore\ F = Mg(\sqrt{2} - 1)$
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