Heating curves
Turning 135 g of ice at −15 °C into steam at 120 °C takes 416 kJ, and 305 kJ of that goes into boiling alone.
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Put a block of ice on a stove that gives heat at a steady rate and record its temperature. The graph of temperature against heat added is a heating curve. It is a staircase. The sloping parts are where one state warms up. The flat parts are where the state changes. On those plateaus the burner keeps adding heat, but the thermometer does not move.
Two formulas
On a sloping part the heat raises the temperature, and the amount follows q = m c ΔT: mass times specific heat times temperature change. Specific heat is the heat needed to warm 1 g by 1 °C. For ice it is 2.09 J/g °C, for liquid water 4.18 J/g °C and for steam 1.86 J/g °C. Liquid water needs about twice as much heat per degree as ice or steam.
On a flat part the heat changes the state, and the amount follows q = n ΔH: moles times enthalpy of the change. To get moles, divide the mass by the molar mass, 18.02 g/mol for water. Melting uses ΔH fusion, 6.01 kJ/mol. Boiling uses ΔH vaporization at the boiling point, 40.67 kJ/mol.
Working through the example
| Step | Formula | Heat |
|---|---|---|
| 1. Ice −15 °C to 0 °C | 135 × 2.09 × 15 | 4.23 kJ |
| 2. Melt at 0 °C | 135 ÷ 18.02 × 6.01 | 45.0 kJ |
| 3. Water 0 °C to 100 °C | 135 × 4.18 × 100 | 56.4 kJ |
| 4. Boil at 100 °C | 135 ÷ 18.02 × 40.67 | 304.7 kJ |
| 5. Steam 100 °C to 120 °C | 135 × 1.86 × 20 | 5.02 kJ |
| Total | 415.4 kJ, about 416 kJ |
The table follows OpenStax. The steps in joules are turned into kilojoules before adding. OpenStax rounds each step and reports 416 kJ; adding unrounded values gives 415.4 kJ, which the lab model above shows. Look at how lopsided the numbers are. Boiling takes almost three quarters of the total, more than five times the 56.4 kJ needed to take the water all the way from 0 °C to 100 °C. On the curve this is the long plateau at 100 °C.
Reading the slopes
The sloping parts are not equally steep. On a slope the temperature rises by q ÷ (m c), so the smaller the specific heat, the steeper the line. Ice (2.09 J/g °C) and steam (1.86 J/g °C) warm about twice as fast per kilojoule as liquid water (4.18 J/g °C). In the lab model the ice and steam sections are short and steep, and the water section is long and gentle. Change the mass and every step grows or shrinks in proportion, so the shape of the curve stays the same and only the heat axis stretches.
The same method answers the reverse question. OpenStax asks how much heat 94.0 g of water at 80.0 °C gives out as it cools, freezes and then cools to ice at −30.0 °C. Cooling the water gives 94.0 × 4.18 × 80.0 = 31.4 kJ, freezing gives 94.0 ÷ 18.02 × 6.01 = 31.4 kJ and cooling the ice gives 94.0 × 2.09 × 30.0 = 5.9 kJ, for 68.7 kJ in all.
What a cook can learn from it
Once a pot of water is boiling, turning the burner up does not make the water hotter. The temperature stays at the boiling point; the extra heat only makes the water boil away faster. Lowering the flame to a gentle boil cooks food at the same temperature and saves fuel. A cooling curve is the same staircase run backwards: steam cools, condenses at 100 °C while giving out heat, water cools, freezes at 0 °C and then the ice cools.
- What does a flat part of a heating curve show?
- A change of state at constant temperature
- The burner has turned off
- The substance is cooling
- Heat to warm 135 g of ice from −15 °C to 0 °C, in joules (c = 2.09 J/g °C)?
- Heat to warm 100 g of liquid water from 20 °C to 100 °C, in kJ (c = 4.18 J/g °C)? 2 decimal places.
- How many moles are in 135 g of water (18.02 g/mol)? 2 decimal places.
- Heat to boil 135 g of water at 100 °C, in kJ (40.67 kJ/mol)? Whole number.
- Which step takes the most heat in the 135 g example?
- Boiling at 100 °C
- Warming water from 0 to 100 °C
- Melting at 0 °C
- Water is boiling hard. You turn the burner up. The water temperature…
- stays at the boiling point
- rises above 100 °C
- drops
- Specific heat of liquid water is 4.18 J/g °C and of ice 2.09 J/g °C. How many times more heat per degree does the water need?
- Total heat to take 18.02 g of ice (1 mol) from −15 °C to steam at 120 °C, in kJ? 1 decimal place.
- Put the steps of the heating curve in order.
- Slopes: q = m c ΔT (ice 2.09, water 4.18, steam 1.86 J/g °C).
- Plateaus: q = n ΔH (6.01 and 40.67 kJ/mol for water).
- 135 g of ice at −15 °C to steam at 120 °C: about 416 kJ, 305 kJ of it for boiling.
- Turning up the heat under boiling water does not raise its temperature.
Sources for this course (8)
- OpenStax Chemistry 2e (openstax.org/books/chemistry-2e): 1.2 Phases and Classification of Matter (matter, three states, plasma, mass and weight, Moon 1/6, conservation of matter, sand and clouds)
- 9.2 gas laws (Boyle's law P1V1 = P2V2, syringe 15.0 mL 13.0 psi to 7.5 mL 26 psi, breathing, divers: every 33 ft of sea water adds 1 atm and halves the air volume at 33 ft, Amontons ~1700, Gay-Lussac ~1800, Charles, STP 273.15 K and 101.325 kPa, -273 °C absolute zero)
- 9.5 kinetic-molecular theory (average kinetic energy proportional to kelvin temperature, KEavg = 3/2 RT, urms = sqrt(3RT/M), N2 at 30 °C 519 m/s, O2 at -23 °C 441 m/s)
- 10.3 phase transitions (vapor pressure, normal boiling point at 1 atm = 101.3 kPa, Leadville 68 kPa about 90 °C, ΔHvap 44.01 kJ/mol at 25 °C and 40.67 kJ/mol at 100 °C, 1.5 L sweat 3600 kJ, ΔHfus 6.01 kJ/mol, ice at -12 °C staying at 0 °C while melting, CO2 sublimation 26.1 kJ/mol, frost is deposition, heating curve example 135 g ice -15 °C to steam 120 °C = 416 kJ with c ice 2.09, water 4.18, steam 1.86 J/g °C, burner turned up does not raise boiling temperature)
- NIST Chemistry WebBook phase change data (webbook.nist.gov: ethanol Tfus 159 K, Tboil 351.5 K; nitrogen Tfus 63.3 K, Tboil 77.34 K; oxygen Tfus 54.8 K, Tboil 90.2 K; mercury Tfus 234.31 K, Tboil 629.81 K; CO2 triple point 216.58 K at 5.185 bar, solid vapour-pressure equation Giauque and Egan 1937 giving 194.7 K at 1 atm)
- USGS Water Science School, Water Density (0.99987 g/cm³ at 0 °C, 1.00000 at 4 °C, 0.95865 at 100 °C; ice about 9% less dense)
- Britannica, Boyle's law (Robert Boyle 1662, air compressed by mercury; Edme Mariotte 1676)
- Boyle's 1662 table (48 spaces at 29 2/16 in, 12 spaces at 117 9/16 in of mercury) as reprinted in J. Appl. Physiol. 87 (1999) 1543.
Checked: 2026-10-17