Q.Calculate the heat required to convert 3 kg of ice at −12 ∘C kept in a calorimeter to steam at 100 ∘C at atmospheric pressure. Given specific heat capacity of ice =2100 J kg−1 K−1, specific heat capacity of water =4186 J kg−1 K−1, latent heat of fusion of ice =3.35×105 J kg−1 and latent heat of steam =2.256×106 J kg−1.
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Specific Heat Capacity
What is Specific Heat Capacity?
Imagine you have two identical stoves, two identical pots, and you put 1 kg of water in one pot and 1 kg of iron in the other. You turn both stoves to the same flame. After 2 minutes, the iron is scorching hot — you can't touch it. The water is still lukewarm.
Why? Because different substances need different amounts of heat to raise their temperature by the same amount. That's the core idea behind specific heat capacity.
The Intuition
Think of heat as "energy currency" and temperature rise as "buying a degree." Some materials are "cheap" — a little heat buys a big temperature rise. Others are "expensive" — you need to spend a lot of heat to get even a small rise.
- Iron is cheap: a small heat input → large temperature jump.
- Water is expensive: a large heat input → small temperature jump.
This "expensiveness" is what we call specific heat capacity. It tells you how much heat energy is needed to raise the temperature of 1 kg of a substance by 1 °C (or 1 K).
The Precise Definition
c=mΔTQ
Where:
- c = specific heat capacity (J/kg·°C or J/kg·K)
- Q = heat energy supplied (J)
- m = mass of the substance (kg)
- ΔT = change in temperature (°C or K)
In words: Specific heat capacity is the amount of heat required to raise the temperature of one kilogram of a substance by one degree Celsius (or one Kelvin).
Key Points to Remember
-
It's a property of the material, not the object. A small iron nail and a giant iron beam have the same c value — but the beam needs more total heat because it has more mass.
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Units matter. Common values:
- Water: c=4186 J/kg⋅°C (or ≈ 4200 J/kg·°C in many problems)
- Iron: c≈450 J/kg⋅°C
- Copper: c≈390 J/kg⋅°C
Notice water's value is about 10 times that of iron — that's why water heats up so slowly compared to metals.
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The formula works both ways. If a substance cools down, it releases the same amount of heat it would absorb to warm up by the same ΔT.
A Common Mistake to Avoid
Don't confuse specific heat capacity (c) with heat capacity (C). Heat capacity is for an entire object: C=mc. A large iron block can have a higher heat capacity than a small cup of water, even though iron's c is much smaller. Always check: are we talking about per kg or for the whole thing?
Worked Example (Exam-Style)
Problem: How much heat is needed to raise the temperature of 2 kg of water from 20 °C to 50 °C? (Take cwater=4200 J/kg⋅°C)
Solution:
- m=2 kg
- ΔT=50−20=30 °C
- c=4200 J/kg⋅°C
Q=mcΔT=2×4200×30=252000 J=252 kJ
Answer: 252 kJ of heat is required.
Why This Matters …
Four steps, each with its own heat: Q=mcΔT for temperature changes, Q=mL for phase changes.
Q1 (warm ice −12°→0°C) =3×2100×12=75,600 J.
Q2 (melt) =3×3.35×105=1,005,000 J.
Q3 (warm water 0°→100°C) =3×4186×100=1,255,800 J.
Q4 (vaporise) =3×2.256×106=6,768,000 J. …
Converting ice at −12∘C to steam at 100∘C takes four separate steps - warming the ice, melting it, warming the water, then vaporising it - and the total heat required is 9.10×106 J.
Ice cannot jump straight to steam; it must pass through every intermediate stage, and each stage needs its own heat calculation: Q=mcΔT for a temperature change, Q=mL for a phase change.
Step 1 - Warm the ice from −12∘C to 0∘C
Q1=mciceΔT=3×2100×12=75,600 J.
Step 2 - Melt the ice at 0∘C
Q2=mLf=3×3.35×105=1,005,000 J.
Step 3 - Warm the water from 0∘C to 100∘C
Q3=mcwaterΔT=3×4186×100=1,255,800 J.
Step 4 - Vaporise the water at 100∘C
Q4=mLv=3×2.256×106=6,768,000 J.
Total
Q=Q1+Q2+Q3+Q4=75,600+1,005,000+1,255,800+6,768,000=9,104,400 J. …
Before adding four terms blind, it's worth noticing which step dominates: vaporising the water (Q4≈6.77×106 J) alone accounts for roughly 74% of the total heat required — far more than melting or either temperature-change step combined. This is the general lesson behind mixed heating/phase-change problems: the latent-heat terms, especially vaporisation, usually dwarf the mcΔT terms, so a quick estimate using …
- COMEDK 2026Set 2026-A1 markMCQQ.A block of a certain material is heated to a temperature of 500∘C and then placed on a large ice block. If 1.455 kg of ice melts, find the mass of the block. Specific heat of the material is 0.39Jg−1C−1 and heat of fusion of water is 335Jg−1. (A) 0.67 kg (B) 2.5 kg (C) 1.455 kg (D) 2.67 kg
›Reveal solutionSolution
The heat lost by the block as it cools from 500°C to 0°C equals the heat gained by the ice to melt. Using the heat balance equation, the mass of the block is found to be 2.5 kg, corresponding to option (B).
Concept and Intuition
When a hot object is placed on ice, the object cools down by transferring heat to the ice. The ice uses that heat to change phase from solid to liquid (melting) at a constant temperature of 0°C. The key principle is conservation of energy: the heat lost by the block equals the heat gained by the ice (assuming no heat loss to the surroundings). The block’s heat loss depends on its mass, specific heat, and temperature change. The ice’s heat gain depends on the mass of ice melted and the latent heat of fusion. By equating these, we can solve for the unknown mass of the block.
Step-by-step solution
- Identify the heat lost by the block The block cools from 500∘C to 0∘C (the melting point of ice). The heat lost is given by:
Qblock=mblock⋅c⋅ΔT
where c=0.39Jg−1∘C−1 and ΔT=500−0=500∘C.
So:
Qblock=mblock×0.39×500
- Identify the heat gained by the ice The ice melts at 0∘C using the latent heat of fusion. The heat gained is:
Qice=mice⋅Lf
where mice=1.455kg=1455g (since specific heat is given in Jg−1, we work in grams) and Lf=335Jg−1.
So:
Qice=1455×335
- Apply conservation of energy Assuming no heat is lost to the environment, the heat lost by the block equals the heat gained by the ice:
mblock×0.39×500=1455×335
- Solve for mblock First, compute the right-hand side:
1455×335=1455×(300+35)=436500+50925=487425
(Alternatively, 1455×335=487425).
The left-hand side simplifies:
0.39×500=195
So the equation becomes:
195mblock=487425
Divide both sides by 195:
mblock=195487425
Perform the division:
195×2500=487500(a bit too high by 75)
So:
mblock=2500−19575=2500−0.3846≈2499.615g
But more precisely:
487425÷195=2500−19575=2500−135≈2499.615
However, note that 195×2500=487500 and 487500−487425=75, so the exact value is 2500−75/195=2500−5/13. But wait—check if the numbers are exact: …
- COMEDK 2026Set 2026-M1 markMCQQ.Two bodies of specific heats C1 and C2, having the same heat capacities are combined to form a single composite body. The specific heat capacity of the composite body is (A) C1−C2 (B) C1+C22C1C2 (C) C1+C2 (D) C1+C22C2
›Reveal solutionSolution
The key is that “same heat capacities” means the two bodies have equal total heat capacity (mass × specific heat), not equal specific heats. Using that constraint, the composite specific heat is the harmonic mean of the two, giving option (B).
The problem is a classic trap: it says “having the same heat capacities.” Many students read that as “same specific heat,” but heat capacity is the product of mass and specific heat: Cbody=mc. So “same heat capacities” means
m1C1=m2C2
where C1 and C2 are the specific heats (per unit mass). The composite body has total mass m1+m2 and total heat capacity m1C1+m2C2. Its specific heat is that total divided by total mass.
- Set up the equality of heat capacities Let the two bodies have masses m1 and m2 and specific heats C1 and C2. Their heat capacities are equal:
m1C1=m2C2
This is the only relation between the masses.
- Express masses in terms of one another From the equality,
m2=C2m1C1
- Total heat capacity of the composite The composite’s total heat capacity is the sum:
Ctotal=m1C1+m2C2
Substitute m2:
Ctotal=m1C1+(C2m1C1)C2=m1C1+m1C1=2m1C1
- Total mass of the composite mtotal=m1+m2=m1+C2m1C1=m1(1+C2C1)=m1C2C1+C2 …
- COMEDK 2024Set 2024-A1 markMCQQ.An iron piece of mass 200 g is kept inside a furnace for some time and then put in a calorimeter of water equivalent 20 g containing 230 g of water at 20C. The steady state temperature attained by the mixture is 60∘. The temperature of the furnace is (Specific heat capacity of iron is 470 J kg−1C−1 ) (A) 464.7∘C (B) 893.6∘C (C) 506.8∘C (D) 953.6∘C
›Reveal solutionSolution
Heat lost by the iron equals heat gained by the water and calorimeter. Solving the balance gives the furnace (initial iron) temperature ≈506.8∘C — option (C).
Convert masses to kg to match the given specific heat unit (J kg−1∘C−1): iron 0.200 kg, water 0.230 kg, calorimeter water-equivalent 0.020 kg (total effective water 0.250 kg). Take water cw=4200 J kg−1∘C−1 and iron c=470.
- Heat gained by water + calorimeter (20→60∘C):
Qgain=0.250×4200×(60−20)=42000 J.
- Heat lost by iron (T→60∘C):
Qlost=0.200×470×(T−60)=94(T−60).
- Energy balance Qlost=Qgain: …
- COMEDK 2024Set 2024-M1 markMCQQ.A one kg block of ice at −1.5∘C falls from a height of 1.5 km and is found melting. The amount of ice melted due to fall, if 60% energy is converted into heat is (Specific heat capacity of ice is 0.5 cal g−1 C−1, Latent heat of fusion of ice =80 cal g−1 ) (A) 1.69 g (B) 10 g (C) 16.9 g (D) 17.9 g
›Reveal solutionSolution
The falling ice loses gravitational potential energy; 60% of that energy becomes heat, which first warms the ice to 0°C and then melts some of it. The mass melted is about 16.9 g, so the correct option is (C).
Concept & Intuition
When the ice falls, its gravitational potential energy is converted into kinetic energy, and upon impact, most of that kinetic energy is dissipated as heat. The problem tells us that 60% of the total mechanical energy becomes thermal energy absorbed by the ice. That heat does two things: it raises the temperature of the entire 1 kg block from –1.5°C to 0°C (sensible heat), and the remaining heat then melts a portion of the ice (latent heat). We need to find how much ice actually melts.
- Calculate the total gravitational potential energy lost The ice has mass m=1 kg=1000 g. Height h=1.5 km=1500 m. Gravitational potential energy:
Epot=mgh=(1 kg)(9.8 m/s2)(1500 m)=14700 J
- Convert this energy into calories Since the specific heat and latent heat are given in calories, we work in calories. 1 cal=4.184 J, so
Epot=4.18414700≈3513.4 cal
- Only 60% of this energy becomes heat
Qavailable=0.60×3513.4≈2108.0 cal
- First, warm the ice from –1.5°C to 0°C Specific heat of ice c=0.5 calg−1°C−1. Mass of ice = 1000 g. Heat needed to raise temperature: Qwarm=mcΔT=(1000)(0.5)(1.5)=750 cal …
- KCET 2018Set A-11 markMCQQ.A cup of tea cools from 65.5∘C to 62.5∘C in 1 minute in a room at 22.5∘C. How long will it take to cool from 46.5∘C to 40.5∘C in the same room? (A) 4 minutes (B) 2 minutes (C) 1 minute (D) 3 minutes
›Reveal solutionSolution
Use Newton's law of cooling in the finite-difference form — rate of fall of temperature ∝ (average temperature of the body − room temperature) — calibrate k from the first observation and use it for the second.
Step 1 — The law and why this form works.
Newton's law of cooling states that the rate of heat loss is proportional to the excess of the body's temperature over its surroundings:
−dtdθ=k(θ−θ0)
When the temperature drop over the interval is small compared with the excess temperature, we may replace θ by the average temperature over the interval:
tθ1−θ2=k(2θ1+θ2−θ0)
Step 2 — Calibrate k from the first cooling.
θ1=65.5∘C, θ2=62.5∘C, t=1 min, θ0=22.5∘C.
θˉ=265.5+62.5=64.0∘C,θˉ−θ0=64.0−22.5=41.5∘C
165.5−62.5=k(41.5)⇒3=41.5k⇒k=41.53 min−1
Step 3 — Apply to the second cooling.
θ1=46.5∘C, θ2=40.5∘C, unknown time t. …
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