A metal block of density 6000 kg m−3 and mass 1.2 kg is suspended through a spring of spring constant 200 N m−1. The spring-block system is dipped in water kept in a vessel. The water has a mass of 260 g and the block is at a height 40 cm above the bottom of the vessel. If the support to the spring is broken, what will be the rise in the temperature of the water? Specific heat capacity of the block is 250 J kg−1 K−1 and that of water is 4200 J kg−1 K−1. Heat capacities of the vessel and the spring are negligible.
Initially, when the block is suspended from the spring inside water it is in mechanical equilibrium. Also, the water and block are in thermal equilibrium. The extension of the spring be x, and m be the mass of the block, ρ density.
k is the spring constant, ρw → density of water
V → volume of block
Net force on the block along the vertical direction is zero, as block is at rest.
∴ kx = mg − ρw vg
⇒ x = mg(1 − ρwρ)k
⇒ kx = 12g − 16 × 1.2 g = g
⇒ x = gk = 10200 = 120 m
Now, after the support breaks, the block falls and hits the floor, and comes to rest, the spring comes to its natural length, gravitational potential energy is lost too.
∴ M.E. lost = 12 kx2 + mgapparentY ............(i)
[gapparent = Gravitational force − Buoyancy forcem
gapparent = Gravitational force − Buoyancy forcem = mg−ρwρmgm = 5g6]
Also, now the water and block have both risen to the equal temperature, higher by ΔT
h→ height block falls, M→ mass of water; sblock, swater the specific heats
∴ Heat gained = (msblock + Mswater)ΔT . . . .(ii)
(i) & (ii) are equal
⇒ DeltaT = 0.003∘C
[Note: Don't think of this as some different concept, remember work - energy theorem problems with dissipative forces (like viscosity in this question) friction etc. The work done by viscous forces here is what appears as heat, and changes the temperature]