Tuesday, 27 February 2018
HC Verma Concepts Of Physics Exercise Solutions Of Chapter 25 (Calorimetry)
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HC
Verma Concepts of Physics Solutions - Part 2, Chapter 25 (Calorimetry):
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EXERCISE
1. An aluminium vessel of
mass 0.5 kg contains 0.2 kg of water at 20°C. A block of iron of mass 0.2 kg at
100°C is gently put into the water. Find the equilibrium temperature of the
mixture. Specific heat capacities of aluminium, iron and water are 910 J/kg-K,
470 J/kg-K and 4200 J/kg-K respectively.
Sol:
Given: Mass of aluminium ma
= 0.5kg; Mass of water mw = 0.2 kg; Mass of Iron mi = 0.2
kg; Temperature of aluminium and water = 20°C = 297 K; Temperature of Iron =
100°C = 373 K; Specific heat of aluminium = 910 J/kg-k; Specific heat of Iron =
470 J/kg-k; Specific heat of water = 4200J/kg-k.
Assumption: heat interaction outside
of the boundary is zero.
∴ Heat loss by iron block = heat gain by aluminium
vessel and water
Or, 0.2 * 470 * (373 – T) = (T – 293)
(0.5 * 910 + 0.2 * 4200)
Or, 94 * (373 – T) = (T – 293) (455 +
840)
Or, 373 – T = (T – 293) * 13.8
Or, T = 298 K = 25 0C.
2. A piece of iron of mass
100 g is kept inside a furnace for a long time and then put in a calorimeter of
water equivalent 10 g containing 240 g of water at 20°C. The mixture attains an
equilibrium temperature of 60°C. Find the temperature of the furnace. Specific
heat capacity of iron = 470 J/kg-°C.
Sol:
Given: mass of iron, miron
= 100 g = 0.1 kg; mass of water, mw = 240 g = 0.24 kg; water
equivalent of calorimeter, meq = 10 g = 0.01 kg; final temp of
mixture, Tf = 600 C; temp of water, Tw = 200
C; Specific heat capacity of iron, Ciron = 470 J/kg-°C; Cw
= 4184 J/kg-°C.
Let the furnace temperature be T.
Now, heat loss by the iron = heat
gain by the water and calorimeter
Or, miron * Ciron
* (T – Tf) = (mw + meq) * Cw * (Tf
– Tw)
Or, 0.1 * 470 * (T – 60) = (0.24
+0.01) * 4184 * (60 – 20)
Or, T = 9500 C.
So, the temperature of the furnace is
9500 C.
3. The temperatures of equal
masses of three different liquids A, B and C are 12°C, 19°C and 28°C
respectively. The temperature when A and B are mixed is 16°C, and when B and C
are mixed, it is 23°C. What will be the temperature when A and C are mixed?
Sol:
Given: TA = 120C;
TB = 190C; TC = 280C; mA
= mB = mC = m; temperature of mixture A and B is 160C;
temperature of mixture B and C is 230C.
For mixture A and B: temperature of
mixture, T = 160C.
→Heat gain by A = heat loss by B
Or, mA CA (T –
TA) = mB CB (TB – T)
Or, m CA (16 – 12) = m CB
(19 – 16)
Or, 4 CA = 3 CB
For mixture B and C: temperature of
mixture, T = 230C.
→Heat gain by B = heat loss by C
Or, mB CB (T –
TB) = mC CC (TC – T)
Or, m CB (23 – 19) = m CC
(28 – 23)
Or, 4 CB = 5 CC
For mixture A and C: temperature of
mixture, T.
→Heat gain by A = heat loss by C
Or, mA CA (T –
TA) = mC CC (TC – T)
Or, m (3/4) CB (T – 12) =
m (4/5) CB (28 – T)
Or, (3/4) (T – 12) = (4/5) (28 – T)
Or, 15 T – 180 = 448 – 16 T
Or, T = 628/31 = 20.30C.
4. Four 2 cm * 2 cm * 2 cm
cubes of ice are taken out from a refrigerator and are put in 200 ml of a drink
at 10°C. (a) Find the temperature of the drink when thermal equilibrium is
attained in it. (b) If the ice cubes do not melt completely, find the amount
melted. Assume that no heat is lost to the outside of the drink and that the
container has negligible heat capacity. Density of ice = 900 kg/m3,
density of the drink = 1000 kg/m3, specific heat capacity of the
drink = 4200 J/kg-K, latent heat of fusion of ice = 3.4 * 105 J/kg.
Sol:
Given: Density of ice, ρi
= 900 kg/m3; specific heat capacity of ice, Ci = 2108
J/kg-K; density of the drink, ρd = 1000 kg/m3; specific
heat capacity of the drink, Cd = 4200 J/kg-K; latent heat of fusion
of ice, L = 3.4 * 105 J/kg; volume of ice, Vi = 4 * 23
= 32 cm3 = 32 * 10-6 m3; volume of drink, Vd
= 200 ml = 2 * 10-4 m3.
Mass of the ice, mi = ρi
Vi = 900 * 32 * 10-6 = 288 * 10-4 kg
Mass of the drink, md = ρd
Vd = 1000 * 2 * 10-4 = 0.2 kg
Heat required to melt ice completely
is
→ Qm = miL = 288
* 10-4 * 3.4 * 105 = 9792 J.
Heat release when drink comes from 100
C to 00 C is
→ Qd = mdCdΔT
= 0.2 * 4200 * (10 – 0) = 8400 J.
Since, Qd is greater than
Qm. So complete ice will not melt.
(a)
The temperature of the drink when thermal equilibrium is attained is 00 C.
(b)
Let the amount ice melt be m.
→ Latent heat of melted ice = Heat
loss by the drink
Or, mL = 8400
Or, 3.4 * 105 * m = 8400
Or, m = 8400/ (3.4 * 105)
= 0.025 kg = 25 g.
5. Indian style of cooling
drinking water is to keep it in a pitcher having porous walls. Water comes to
the outer surface very slowly and evaporates. Most of the energy needed for
evaporation is taken from the water itself and the water is cooled down. Assume
that a pitcher contains 10 kg of water and 0.2 g of water comes out per second.
Assuming no backward heat transfer from the atmosphere to the water, calculate
the time in which the temperature decreases by 5°C. Specific heat capacity of
water = 4200 J/kg-°C and latent heat of vaporization of water = 2.27 * 106
J/kg.
Sol:
Given: mass of water, mw =
10 kg; Cw = 4200 J/kg-°C; latent heat of vaporization, L = 2.27 * 106
J/kg; rate at which water comes, m’ = 0.2 g/s = 0.2 * 10-3 kg/s; ΔT
= 50 C. let time = t.
According to the question,
→ Heat loss by the water = latent
heat of vaporization of water
Or, mw * Cw *
ΔT = m’ * t * L
Or, 10 * 4200 * 5 = 0.2 * 10-3
* 2.27 * 106 * t
Or, t = 462.55 s = 7.7 min.