Latent heat
When you heat a pot of water on the stove, the temperature rises until it starts to boil. Then it stays at 100 °C although the flame is still giving heat. Where does the heat go? It is used up in changing water into steam.
Latent heat (सुप्त उष्णता) is the heat absorbed or given out during a change of state without any change of temperature.
Rule 1: Latent heat of fusion and vapourization — While ice melts at 0 °C or water boils at 100 °C, heat is absorbed but the temperature stays constant, because the heat is used to break the bonds between particles. Heat absorbed during melting is the latent heat of fusion; during boiling it is the latent heat of vapourization.
In the figure : In the figure temperature stays constant while the state changes.
- Easy : A mixture of ice and water stays at 0 °C while the ice is melting, even in a warm room.
- Medium : Boiling water in an open pan stays at 100 °C; turning up the flame only makes it boil faster, not hotter.
- Exam-type : Steam at 100 °C burns more than boiling water at 100 °C because every kilogram of steam carries an extra 2256 kJ of latent heat that it gives to the skin when it condenses.
Rule 2: Specific latent heat — Specific latent heat (विशिष्ट सुप्त उष्णता) is the heat absorbed by unit mass at constant temperature during a change of state: Q = m L. For water and ice: fusion 333 kJ/kg (80 cal/g); vapourization 2256 kJ/kg (540 cal/g). The values depend on atmospheric pressure.
- Easy : Melting 2 kg of ice at 0 °C: Q = 2 × 333 = 666 kJ.
- Medium : Turning 50 g of boiling water at 100 °C into steam: Q = 50 × 540 = 27,000 cal.
- Exam-type : Heat needed to turn 1 kg of ice at 0 °C into steam at 100 °C: melt 333 kJ + warm water (1 × 4.18 × 100 = 418 kJ) + vapourize 2256 kJ = 3007 kJ.
During a change of state the temperature is constant. Fusion 333 kJ/kg (80 cal/g); vapourization 2256 kJ/kg (540 cal/g).
Thinking the temperature keeps rising while ice melts. It stays at 0 °C until all ice has melted.
Memory clue: "Melting 80, boiling 540 (calories per gram)".
Spot the difference
| Change | Latent heat | Value |
|---|---|---|
| Ice to water | Fusion | 333 kJ/kg |
| Water to steam | Vapourization | 2256 kJ/kg |
Practice questions
- 1What is latent heat?
- 2State the specific latent heat of fusion of ice.
- 3What is the specific latent heat of vapourization of water?
- 4What is the temperature of boiling water in an open vessel at sea level?
- 5Find the heat needed to melt 5 kg ice at 0 °C.
- 6Find the heat needed to melt 30 g ice at 0 °C in calories.
- 7Why does steam cause a worse burn than boiling water at the same temperature?
- 8Why does the temperature of a boiling kettle not rise even if heating continues?
Show answers (try them yourself first)
- 1Heat absorbed or released during a change of state at constant temperature.
- 2333 kJ/kg (80 cal/g).
- 32256 kJ/kg (540 cal/g).
- 4100 °C.
- 55 × 333 = 1665 kJ.
- 630 × 80 = 2400 cal.
- 7When steam condenses it gives up its large latent heat to the skin.
- 8All the extra heat goes into changing water into steam, not into raising the temperature.
Regelation and anomalous behaviour of water
Press two ice cubes together hard and they stick; ice melts a little under the pressure and freezes again when the pressure is removed. And in winter, a lake freezes from the top, so fish stay alive underneath. Water behaves in unusual ways.
Regelation (पुनर्हिमायन) is melting under pressure and freezing again when the pressure is removed.
Rule 1: Regelation — Pressure lowers the melting point of ice below 0 °C, so ice melts under pressure and re-freezes when the pressure is removed. A weighted wire slowly passes through an ice slab without cutting it into two pieces. An ice-ball is made by pressing snow.
In the figure : In the figure regelation of ice.
- Easy : Squeezing a snowball melts a thin layer of snow, which freezes again and binds the snow.
- Medium : A skater glides on a thin film of water made by the pressure of the blade.
- Exam-type : In the wire experiment the wire passes through the block and the block is still one piece, because the water above the wire freezes again.
Rule 2: Anomalous behaviour of water — From 0 °C to 4 °C water contracts on heating, so its volume is minimum and its density is maximum at 4 °C. This can be studied with Hope's apparatus. Because of this, aquatic life survives under frozen lakes. But water expands on freezing, so pipes and rocks crack in cold regions.
In the figure : In the figure anomalous expansion of water.
- Easy : Cold water below 4 °C is lighter, so it rises and freezes at the top of the lake.
- Medium : The bottom of a frozen lake stays near 4 °C, where the water is densest, so fish survive.
- Exam-type : A glass bottle full of water kept in a freezer cracks because water expands by about 9% when it turns into ice.
Pressure lowers the melting point of ice. Water has maximum density at 4 °C. Water expands on freezing.
Thinking water contracts all the way down to 0 °C. Below 4 °C it expands as it cools.
Memory clue: "Four degrees is the densest; the top freezes first".
Spot the difference
| Temperature | Behaviour of water |
|---|---|
| 0 °C to 4 °C | Contracts on heating |
| At 4 °C | Maximum density |
| Above 4 °C | Expands on heating |
Practice questions
- 1What is regelation?
- 2At what temperature is the density of water maximum?
- 3Which apparatus shows the anomalous expansion of water?
- 4How does pressure change the melting point of ice?
- 5Why do water pipes burst in very cold regions?
- 6How does a weighted wire pass through an ice block without cutting it?
- 7A 1000 cm³ of water freezes into ice. About what volume does the ice have?
- 8Explain why fish survive in a frozen lake.
Show answers (try them yourself first)
- 1Melting under pressure and freezing again when pressure is removed.
- 24 °C.
- 3Hope's apparatus.
- 4It lowers it below 0 °C.
- 5Water expands when it freezes.
- 6Ice below the wire melts under pressure and the water above the wire freezes again.
- 7About 9% more, around 1090 cm³.
- 8Water at 4 °C is densest and stays at the bottom, and the ice on top insulates the lake, so the water below stays liquid.
Dew point and humidity
On a hot summer day sweat does not dry easily when the air is damp, and you feel sticky. Dry air takes up your sweat fast. How much water vapour is in the air makes the weather feel dry or humid.
Humidity (आर्द्रता) is the moisture, or water vapour, present in the air.
Rule 1: Saturated air and dew point — Air is saturated when it holds the maximum water vapour possible at that temperature: 49 g/kg at 40 °C and 14.7 g/kg at 20 °C. The temperature at which unsaturated air becomes saturated on cooling is the dew point (दवबिंदू).
In the figure : In the figure saturation depends on temperature.
- Easy : Warm air can hold more vapour than cold air: 49 g/kg at 40 °C against 14.7 g/kg at 20 °C.
- Medium : Air at 40 °C that holds 14.7 g/kg of vapour is cooled; at 20 °C it becomes saturated, so its dew point is 20 °C.
- Exam-type : Dew forms on a cold glass of water when the glass is below the dew point of the air around it; the vapour condenses on it.
Rule 2: Absolute and relative humidity — Absolute humidity = mass of vapour per unit volume of air (kg/m³). Relative humidity = (actual mass of vapour ÷ mass needed for saturation at that temperature) × 100. At the dew point it is 100%. Above 60% the air feels humid; below 60% it feels dry.
- Easy : Air at 20 °C holds 7.35 g/kg of vapour: relative humidity = 7.35 ÷ 14.7 × 100 = 50%.
- Medium : Air at 40 °C holding 24.5 g/kg: RH = 24.5 ÷ 49 × 100 = 50% too, though it holds more vapour; relative humidity depends on the temperature.
- Exam-type : A room at 20 °C has air with 14.7 g/kg of vapour. Its RH is 100% and it is at the dew point, so water drops can form on a cold wall.
Warm air holds more vapour. RH = actual ÷ saturation × 100; 100% at the dew point.
Thinking high temperature means high humidity. Humidity depends on the vapour present compared with what the air can hold.
Memory clue: "RH = what it has ÷ what it can hold".
Spot the difference
| Term | Meaning |
|---|---|
| Absolute humidity | Vapour mass per m³ |
| Relative humidity | Actual ÷ saturation × 100 |
| Dew point | Temperature at which air becomes saturated |
Practice questions
- 1What is humidity?
- 2What is the dew point?
- 3What is the relative humidity at the dew point?
- 4Write the formula for relative humidity.
- 5Air at 20 °C holds 11.76 g/kg of vapour (saturation 14.7 g/kg). Find RH.
- 6Air at 40 °C has 9.8 g/kg (saturation 49 g/kg). Find RH and say if it feels humid or dry.
- 7Why do water drops appear on the outside of a cold bottle?
- 8Why does the same amount of vapour give a lower RH on a hotter day?
Show answers (try them yourself first)
- 1Water vapour present in the air.
- 2The temperature at which unsaturated air becomes saturated on cooling.
- 3100%.
- 4RH = (actual vapour mass ÷ saturation vapour mass) × 100.
- 511.76 ÷ 14.7 × 100 = 80%.
- 69.8 ÷ 49 × 100 = 20%; dry.
- 7The air near the bottle is cooled below its dew point and the vapour condenses.
- 8Hot air can hold more vapour, so the actual amount is a smaller fraction of the saturation amount.
Units of heat and specific heat capacity
A big pan of water takes much longer to heat than the same mass of oil, and sand at the beach gets burning hot while the sea stays cool. Different materials need different amounts of heat to warm up.
Specific heat capacity (विशिष्ट उष्माधारकता) c is the heat needed to raise the temperature of unit mass by 1 °C.
Rule 1: Units of heat — The units of heat are the joule (SI) and the calorie. 1 cal is the heat needed to warm 1 g of water by 1 °C, from 14.5 °C to 15.5 °C. 1 kcal = 1000 cal, and 1 cal = 4.18 J. The joule is named after James Prescott Joule.
- Easy : 3 cal = 3 × 4.18 = 12.54 J.
- Medium : 2 kcal = 2000 cal = 2000 × 4.18 = 8360 J.
- Exam-type : A food packet says 250 kcal. In joules: 250 × 1000 × 4.18 = 1,045,000 J = 1045 kJ.
Rule 2: Q = m c ΔT — Heat absorbed or lost Q = m c ΔT. SI unit of c is J/kg °C; CGS unit is cal/g °C. Water has c = 1.0 cal/g °C, which is high.
In the figure : In the figure heat needed to warm water.
- Easy : Heat 200 g of water from 20 °C to 70 °C: Q = 200 × 1 × 50 = 10,000 cal.
- Medium : The same in joules: 10,000 × 4.18 = 41,800 J, or 10 kcal.
- Exam-type : 500 g of copper (c = 0.09 cal/g °C) is heated by 50 °C: Q = 500 × 0.09 × 50 = 2250 cal, much less than water would need (500 × 1 × 50 = 25,000 cal).
Units of heat and specific heat capacity
In the app you can move this figure with your finger.
Open in the app1 cal = 4.18 J. Q = m c ΔT. Water has high specific heat.
Using the final temperature instead of the change ΔT. ΔT = final − initial.
Memory clue: "Q = m c ΔT: mass, material, change".
Spot the difference
| Substance | c (cal/g °C) |
|---|---|
| Water | 1.0 |
| Copper | about 0.09 |
Practice questions
- 1What is the SI unit of heat?
- 2How many joules are in 1 cal?
- 3Define specific heat capacity.
- 4Write the formula for heat absorbed.
- 5Convert 5 kcal into joules.
- 6Find the heat needed to warm 400 g of water from 25 °C to 60 °C.
- 72 kg of a metal (c = 400 J/kg °C) cools from 80 °C to 30 °C. Find the heat lost.
- 8Why does the sea stay cooler than beach sand in the afternoon?
Show answers (try them yourself first)
- 1Joule.
- 24.18 J.
- 3Heat needed to raise the temperature of unit mass by 1 °C.
- 4Q = m c ΔT.
- 55 × 1000 × 4.18 = 20,900 J.
- 6400 × 1 × 35 = 14,000 cal.
- 72 × 400 × 50 = 40,000 J.
- 8Water has a high specific heat, so it needs much more heat to rise in temperature.
Principle of heat exchange and calorimetry
When you add cold milk to hot tea, the tea cools and the milk warms until both are at the same temperature. The heat the tea lost is exactly what the milk gained. That is the principle of heat exchange.
Principle of heat exchange (उष्णता विनिमयाचे तत्त्व): heat lost by the hot body = heat gained by the cold body, in an isolated system.
Rule 1: Principle and calorimeter — In an isolated system, heat lost by the hot object equals heat gained by the cold object. In the mixing method with a calorimeter (उष्णतामापक), heat lost by the hot solid = heat gained by the water + heat gained by the calorimeter.
In the figure : In the figure heat lost equals heat gained.
- Easy : Mix 100 g of water at 80 °C with 100 g of water at 20 °C: the final temperature is the middle value, 50 °C.
- Medium : Mix 200 g of water at 60 °C with 300 g at 20 °C: 200 × (60 − T) = 300 × (T − 20), so 12,000 − 200T = 300T − 6000; 18,000 = 500T; T = 36 °C.
- Exam-type : A 150 g metal ball (c = 0.2 cal/g °C) at 100 °C goes into 300 g of water at 20 °C: 150 × 0.2 × (100 − T) = 300 × 1 × (T − 20); 3000 − 30T = 300T − 6000; 9000 = 330T; T ≈ 27.3 °C.
Heat lost = heat gained. Final temperature lies between the two starting temperatures.
Forgetting that the calorimeter also gains heat. Include its share.
Memory clue: "Hot loses, cold gains, balance at the middle".
Spot the difference
| Object | Heat |
|---|---|
| Hot body | Loses |
| Cold body | Gains |
| Isolated system | Lost = gained |
Practice questions
- 1State the principle of heat exchange.
- 2What is a calorimeter used for?
- 3Heat needed to warm 5 kg of water from 20 °C to 100 °C (c = 1 kcal/kg °C)?
- 4Mix 50 g of water at 90 °C with 50 g at 30 °C. Find T.
- 5Mix 100 g at 70 °C with 400 g at 20 °C (water). Find T.
- 6Will 100 g of ice at 0 °C melt completely in 200 g of water at 40 °C (no losses)?
- 7Why must the calorimeter be insulated?
- 8Why is the final temperature always between the two starting temperatures?
Show answers (try them yourself first)
- 1Heat lost by the hot body equals heat gained by the cold body.
- 2Measuring heat in mixing experiments.
- 35 × 1 × 80 = 400 kcal.
- 460 °C.
- 5100 × (70 − T) = 400 × (T − 20); 7000 − 100T = 400T − 8000; T = 30 °C.
- 6Heat available = 200 × 1 × 40 = 8000 cal; heat needed = 100 × 80 = 8000 cal; so it just melts completely and the mixture is at 0 °C.
- 7To prevent heat loss to the surroundings, so the system is isolated.
- 8The hot body cools and the cold body warms until they reach equal temperature, so neither goes beyond the other's starting value.
Quick revision
- Latent heat: no temperature change during phase change.
- Water: maximum density at 4 °C.
- Q = m c ΔT; 1 cal = 4.18 J.