Heating Curves & Phase-Change Energy — Print · Grade 11 Science

Chapter: States of Matter & Gases

Heating Curves & Phase-Change Energy

Learning goals

Readings for this unit

Before this unit

Energy, temperature, phase changes, and multiplication with units.

Use the detailed parent plan: two core 50–60-minute sessions per focused unit, with a third assigned for selected calculation/modeling topics. First study the core explanation and Parts 1–2 with their figures/checks; next study Parts 3–4, the whole-unit application, worked cases, varied practice and exit check. Attempt reasoning before opening guidance. Extend time when actual understanding requires it; investigations and chapter assessments have separate sessions.

Start with something to explain

Can a thermometer stay steady while the heater keeps transferring energy?

Illustrative evidence case. A selected ice–water mixture melts at nearly constant temperature under fixed pressure.

A heating curve distinguishes temperature change from phase conversionA heating curve distinguishes temperature change from phase conversionTemperature (°C)05010003712Time under selected heating program (relative)Plateaus: phase mixture; slopes: warming within one phase.
Original qualitative program for a selected pure-substance model. Relative time lengths are not a calibrated water-heating experiment or a constant-power claim.

Notice and wonder

Record two observations using the stated quantities or relationships. Keep observations separate from possible causes. Write one question that a new measurement could help answer.

Can a thermometer stay steady while the heater keeps transferring energy?

Your first model

Track phase fraction separately from temperature and energy input.

Build the language from the idea

latent heat
Energy per unit mass for a specified phase change.
plateau
A section where temperature remains nearly constant while energy changes phase.

Heating a substance can raise temperature or change its phase. Temperature measures the average kinetic-energy scale of particles; internal energy also includes interactions and other microscopic motion. During melting or boiling at constant pressure, a pure substance can absorb energy while its temperature stays approximately constant.

Within one phase, q = mcΔT estimates transferred heat when specific heat is approximately constant. During a phase change, use q = mL, where L is specific latent heat, or q = nΔHphase when molar phase-change enthalpy is supplied. These are different relationships; a zero ΔT does not mean zero transferred energy.

Sensible heating uses mass, specific heat and a temperature differenceSensible heating uses mass, specific heat and a temperature differenceq = mcΔT10.0 g × 4.18 J/(g·°C) × 20.0°C= 836 JUse this expression within the stated single liquid phase.
Original 10.0 g water warming calculation under a supplied specific-heat approximation, not measured calorimetry.

A heating curve plots temperature against time or supplied energy. Sloping sections correspond to heating within a phase, and plateaus correspond to coexistence during transitions under the chosen conditions. Equal time intervals represent equal energy input only if heating power is constant and heat loss is negligible.

A heating curve distinguishes temperature change from phase conversionA heating curve distinguishes temperature change from phase conversionTemperature (°C)05010003712Time under selected heating program (relative)Plateaus: phase mixture; slopes: warming within one phase.
Original qualitative program for a selected pure-substance model. Relative time lengths are not a calibrated water-heating experiment or a constant-power claim.

For a multistage calculation, find each contribution and add: warm ice, melt it, warm liquid water, vaporize it, warm vapor if needed. Use a phase-appropriate specific heat and the stated pressure. Water boils near 100°C at 1 atm; changing pressure changes its boiling temperature.

Add stages without using one formula across different processesAdd stages without using one formula across different processesStage for 10.0 g ice at 0°CEnergy to sampleMelt at 0°C3340 JWarm liquid from 0°C to 20°C836 JTotal idealized input4176 J ≈ 4.18 kJA multi-stage account adds different physical processes.
Original idealized two-stage water account with rounded constants; the total is sample energy, not a prediction of an appliance’s electrical consumption.

On cooling, energy flows out of the sample. Freezing and condensation release latent energy. The microscopic interpretation is that particles settle into arrangements of lower potential energy, transferring the difference to surroundings. Bonds within water molecules generally remain during these ordinary phase changes.

A real curve may slope through an apparent plateau because of heat loss, impurities, sensor position, or incomplete thermal equilibrium. Compare the ideal model with evidence and report those differences. Use supplied high-temperature data at home rather than boiling sealed containers.

Build your understanding

Use the detailed parent plan: two core 50–60-minute sessions per focused unit, with a third assigned for selected calculation/modeling topics. First study the core explanation and Parts 1–2 with their figures/checks; next study Parts 3–4, the whole-unit application, worked cases, varied practice and exit check. Attempt reasoning before opening guidance. Extend time when actual understanding requires it; investigations and chapter assessments have separate sessions.

Part 1 · Separate warming segments from phase-change segments

A heating curve tracks temperature as energy is supplied under specified pressure and heating conditions. Sloped segments can represent warming within one phase; a plateau can represent coexistence while energy changes phase fraction. Constant temperature does not mean no energy transfer. The selected time trace is qualitative: segment durations depend on mass, heating power and energy requirements. Real mixtures, heat loss and changing pressure can blur or shift transitions, so a flat segment is interpreted using the material and experimental context.

A heating curve distinguishes temperature change from phase conversionA heating curve distinguishes temperature change from phase conversionTemperature (°C)05010003712Time under selected heating program (relative)Plateaus: phase mixture; slopes: warming within one phase.
Original qualitative program for a selected pure-substance model. Relative time lengths are not a calibrated water-heating experiment or a constant-power claim.

Read the visual model

Identify the labeled structures and units, then trace the arrows or compare values under the caption’s stated conditions. Separate the displayed evidence from a further inference. Write your reasoning before opening the guidance.

Why can energy continue entering a sample during a constant-temperature plateau?

Visual reasoning — after your attempt

It can change the phase fraction and intermolecular energy account rather than increase mean thermal motion represented by temperature.

For a pure substance at fixed pressure, rising heating-curve segments represent temperature changes within a phase. Nearly flat melting or boiling segments can represent phase conversion while energy enters. A time graph’s slope also depends on heater power and losses, so the graph is not solely a property of the substance.

Label phase composition on each segment rather than assuming every flat portion means the heater stopped. Mixtures can change phase over a temperature range.

Pause and explain

What conditions support a sharp phase-change plateau?

Check your reasoning after answering

A suitable pure substance, approximately fixed pressure, and controlled energy transfer support the simple plateau model; real mixtures and uneven heating can differ.

Part 2 · Use specific heat for a temperature change

Specific heat c relates heat transfer to mass and temperature change within a specified phase and range: q=mcΔT. A temperature difference has the same numerical size in kelvin and Celsius, even though absolute-temperature ratios require kelvin. The selected liquid-water approximation uses 4.18 J/(g·°C); c is not identical for ice and vapor or constant over every condition. Include the sign of ΔT and the system boundary, and do not apply this equation to the latent-energy part of a phase transition.

Sensible heating uses mass, specific heat and a temperature differenceSensible heating uses mass, specific heat and a temperature differenceq = mcΔT10.0 g × 4.18 J/(g·°C) × 20.0°C= 836 JUse this expression within the stated single liquid phase.
Original 10.0 g water warming calculation under a supplied specific-heat approximation, not measured calorimetry.

Read the visual model

Identify the labeled structures and units, then trace the arrows or compare values under the caption’s stated conditions. Separate the displayed evidence from a further inference. Write your reasoning before opening the guidance.

Would using ΔT=0 during melting prove the melting energy is zero?

Visual reasoning — after your attempt

No. The sensible-heating relation does not describe the phase-change energy; use the appropriate latent-energy account.

For a segment without phase change, q=mcΔT with the supplied specific heat and conditions. Use ΔT rather than final temperature alone. A Celsius temperature difference has the same numerical size as a Kelvin difference, though absolute gas temperatures need Kelvin.

For 10 g water warming by 20°C with c=4.18 J/g·°C, q=836 J. A phase-change stage must be calculated separately.

Pause and explain

Why cannot q=mcΔT calculate melting energy at constant temperature?

Check your reasoning after answering

ΔT can be zero while phase change still requires energy. Use the supplied latent heat relationship for that stage.

Part 3 · Use latent energy for conversion

A specific latent energy L gives energy per mass for a particular phase change under specified conditions. Near ordinary-pressure melting, water’s fusion value is about 334 J/g. Melting ten grams of ice at its transition therefore needs about 3,340 J even while temperature is nearly constant. Vaporization has a different value, and reverse transitions have the opposite system heat sign. The energy concerns the full phase arrangement, not ordinary cleavage of every O–H covalent bond in the molecules.

Latent energy changes phase fraction at the stated transitionLatent energy changes phase fraction at the stated transitionqphase = mL10.0 g ice × 334 J/g = 3340 JTemperature can remain near 0°C while melting.L depends on the substance, transition and pressure.
Original rounded water fusion example; it assumes the starting ice is already at the transition temperature and does not include container or environmental losses.

Read the visual model

Identify the labeled structures and units, then trace the arrows or compare values under the caption’s stated conditions. Separate the displayed evidence from a further inference. Write your reasoning before opening the guidance.

Which sign describes heat for the sample during freezing if melting the same amount requires +3340 J?

Visual reasoning — after your attempt

Approximately −3340 J for the reverse transition under the corresponding conditions.

For a supplied mass-specific latent heat L, phase-change energy is q=mL. With a molar enthalpy use moles instead. Match the amount unit to the latent-energy unit. Energy may change particle interactions without increasing temperature, so heat input and temperature rise are not equivalent.

Melting 5 g ice with L=334 J/g requires 1670 J in the model, even at constant melting temperature.

Pause and explain

What is the unit check for q=mL?

Check your reasoning after answering

Grams multiply J/g to give joules. A molar latent enthalpy instead requires moles times J/mol.

Part 4 · Add stages and define system signs

A multi-stage energy calculation separates warming, phase conversion and any additional warming after the transition. For ten grams of ice initially at 0°C and liquid water finally at 20°C, add fusion energy and liquid sensible heat. A real heater supplies more than this ideal sample-only sum when the container warms or energy escapes. State starting and final phase, temperature and pressure, then draw an ordered stage account to avoid double-counting or omitting latent energy.

Add stages without using one formula across different processesAdd stages without using one formula across different processesStage for 10.0 g ice at 0°CEnergy to sampleMelt at 0°C3340 JWarm liquid from 0°C to 20°C836 JTotal idealized input4176 J ≈ 4.18 kJA multi-stage account adds different physical processes.
Original idealized two-stage water account with rounded constants; the total is sample energy, not a prediction of an appliance’s electrical consumption.

Read the visual model

Identify the labeled structures and units, then trace the arrows or compare values under the caption’s stated conditions. Separate the displayed evidence from a further inference. Write your reasoning before opening the guidance.

Why is mcΔT for liquid water alone insufficient for this ice-to-liquid example?

Visual reasoning — after your attempt

It includes only the final liquid warming, omitting the energy needed to melt the initial ice.

Split a process into warming, conversion, and further warming as needed, then add energy contributions. q is positive for energy absorbed by the chosen sample and negative for released energy. Container heating and losses can require more input than the calculated sample-only amount.

Warming ice to its melting point, melting it, and warming liquid water are three different stages with appropriate constants.

Pause and explain

Why can heater input exceed calculated sample absorption?

Check your reasoning after answering

The container and surroundings can also gain energy, and losses may occur. The sample-only calculation is not a complete apparatus energy account.

Apply the whole unit · Melt ice and warm the liquid

Illustrative sample: 10.0 g ice initially at 0°C melts completely then liquid warms to 20°C. Use Lfus=334 J/g and cwater=4.18 J/g·°C; neglect losses and container heating.

Your task

Sketch the two stages, calculate each energy contribution and total, and explain which part can occur without temperature rise. State how a real heater-input measurement could differ.

What your response should show

  • Choose the appropriate chemical model or relationship and state its conditions.
  • Show substitutions, units, particle or charge counts, and intermediate reasoning as relevant.
  • Use supplied evidence to justify the conclusion; distinguish observation from inference.
  • Identify a meaningful limitation, uncertainty, or next measurement.
Response guidance — after your attempt
  1. Melting: q₁=10.0×334=3340 J.

  2. Liquid warming: q₂=10.0×4.18×20=836 J.

  3. Total sample absorption=4176 J≈4.18 kJ with sensible precision.

Melting absorbs energy while temperature remains near 0°C in the stated pure-substance/fixed-pressure model; further input warms the liquid. The positive total describes sample absorption. Actual heater input can exceed it through container heating and environmental loss, so the model should not be mistaken for a measured device efficiency.

Scientific references and source-model foundations

Parent / teacher teaching notes

Require a labeled stage diagram before selecting formulas. Keep mass-specific and molar latent-energy units distinct. Ask the learner to explain each particle symbol, axis, unit and arrow before calculating. Distinguish hypothetical models and calculated curves from measured records. Public OpenSciEd excerpts here are selected foundation prompts, not complete high-school teacher editions or an endorsement. All required advanced explanations and practice are provided locally.

Energy changes during melting and warmingMelting at 0°CLiquid warmsAdded energy (J) →T(°C)10 g ice model3340 J
For 10 g ice initially at 0°C, 3340 J melts it at nearly constant temperature; further energy warms liquid water. Curve is schematic at fixed pressure.

The key idea

Add the energy for each temperature change and each phase change separately.

Worked examples

Example 1

Melt 10.0 g ice at 0°C then warm it to 20°C; Lf=334 J/g and cwater=4.18 J/g°C.
  1. Melting:10×334=3340 J.
  2. Warming:10×4.18×20=836 J.
  3. Add contributions.
Answer: 4176 J, about 4.18 kJ

Example 2 · Worked application

Heat 50 g liquid by 10°C using c=4.0 J/(g·°C), then melt 5 g of a separate solid with L=200 J/g. Find each energy.
  1. Sensible heating: Q=mcΔT=50×4.0×10=2000 J.
  2. Melting: Q=mL=5×200=1000 J.
  3. The second process uses phase-change energy rather than temperature change.
Answer: 2000 J and 1000 J for the stated separate processes.
Check the reasoning

Do not apply mcΔT alone to a phase-change plateau.

Example 3

Why does boiling water not keep warming under fixed pressure?
  1. Energy is still being transferred.
  2. It largely separates molecules into gas during phase coexistence.
Answer: Phase-change energy increases internal energy without a comparable temperature rise.

Example 4 · Find and fix the mistake

Context: Heat 50 g liquid by 10°C using c=4.0 J/(g·°C), then melt 5 g of a separate solid with L=200 J/g. Find each energy. A student claims: “Zero temperature change means zero heating energy.” Evaluate the claim and write a corrected explanation.
  1. Test the claim against the stated conditions: Do not apply mcΔT alone to a phase-change plateau.
  2. Latent energy can change phase without increasing temperature.
Answer: Latent energy can change phase without increasing temperature.
Check the reasoning

Do not apply mcΔT alone to a phase-change plateau.

Example 5 · Reason from the visual model

Latent energy changes phase fraction at the stated transitionLatent energy changes phase fraction at the stated transitionqphase = mL10.0 g ice × 334 J/g = 3340 JTemperature can remain near 0°C while melting.L depends on the substance, transition and pressure.
Original rounded water fusion example; it assumes the starting ice is already at the transition temperature and does not include container or environmental losses.
Which sign describes heat for the sample during freezing if melting the same amount requires +3340 J?
  1. A specific latent energy L gives energy per mass for a particular phase change under specified conditions. Near ordinary-pressure melting, water’s fusion value is about 334 J/g. Melting ten grams of ice at its transition therefore needs about 3,340 J even while temperature is nearly constant. Vaporization has a different value, and reverse transitions have the opposite system heat sign. The energy concerns the full phase arrangement, not ordinary cleavage of every O–H covalent bond in the molecules.
  2. Approximately −3340 J for the reverse transition under the corresponding conditions.
Answer: Approximately −3340 J for the reverse transition under the corresponding conditions.
Check the reasoning

Original rounded water fusion example; it assumes the starting ice is already at the transition temperature and does not include container or environmental losses.

Avoid these mistakes

Check your understanding

Compare sensible and latent heat.

Discuss the answer

Sensible heat changes temperature within a phase; latent heat changes phase at approximately constant temperature under stated conditions.

Return to the phenomenon

Return to the initial case. Can a thermometer stay steady while the heater keeps transferring energy? Revise your drawing or explanation using two named ideas and one stated limitation.

Compare explanations after your attempt

Energy can alter the phase composition at the transition. Divide the full process into latent and sensible stages rather than treating temperature as a direct total-energy meter.

What should we investigate next?

Which comparison would test a remaining uncertainty? State what you would change, keep comparable and measure.

Investigate, calculate and revise

Keep a first model and an evidence-supported revision. Attempt each task before opening guidance; all required explanations and supplied-data routes are available locally.

Activity 1 · Return to the opening case

Assigned reading and preparation

Use the opening phenomenon, unit definitions and explained Parts 1–4.

Your task

Return to the initial case. Can a thermometer stay steady while the heater keeps transferring energy? Revise your drawing or explanation using two named ideas and one stated limitation.

Success criteria

  • Use the stated observations and appropriate units.
  • Connect a labeled model with the chemical mechanism.
  • State assumptions and an evidence limitation.
  • Explain a substantive revision or next test.
Hint

Keep species identity, material transfer and energy account distinct.

Response guidance — discuss after your attempt

Energy can alter the phase composition at the transition. Divide the full process into latent and sensible stages rather than treating temperature as a direct total-energy meter.

Activity 2 · Transfer to a changed case

Assigned reading and preparation

Cover the worked answer and use the explained models, relationships and notebook.

Your task

For 20.0 g ice already at 0°C, calculate energy to melt it and warm the liquid to 10.0°C. Use Lf=334 J/g and c=4.18 J/(g·°C), neglecting apparatus/losses.

Success criteria

  • Use the stated measurements or conditions, with correct units.
  • Connect the result to the chemical mechanism or evidence relationship.
  • Identify the assumption, model limit or further evidence requested.
Hint

Name known quantities and conditions, show intermediate steps and check conservation.

Response guidance — discuss after your attempt

Melting: 20.0×334=6680 J. Warming: 20.0×4.18×10.0=836 J. Total=7516 J≈7.52 kJ. The sample receives positive heat under the stated boundary.

Words to know

latent heat
Energy per unit mass for a specified phase change.
plateau
A section where temperature remains nearly constant while energy changes phase.

In the real world

Use the chapter investigation to connect this unit to measured evidence and a practical decision.

Exit check

Compare sensible and latent heat.

Check your explanation after answering

Sensible heat changes temperature within a phase; latent heat changes phase at approximately constant temperature under stated conditions.

Explain your reasoning without notes. If a key idea is missing, revisit the lesson and try again.

Problem 1

Melt 5 g ice at 0°C using Lf=334 J/g.
Hints

Write the relationship first; substitute with consistent units.

Answer and explanation

1670 J

mL=5×334.

Problem 2

Why is q=mcΔT insufficient across a melting plateau?
Answer and explanation

It includes sensible heating but omits latent heat needed to change phase.

Response criteria

  • State a scientifically accurate conclusion.
  • Show the calculation or mechanism that supports it.
  • Include units, conditions, or limits where relevant.

Problem 3

Freeze 3 g water at its freezing point using Lf=334 J/g. Find heat released as a positive magnitude.
Hints

List the given quantities, select a relationship, and check units before substituting.

Answer and explanation

1002 J

3×334=1002; sample heat would be negative.

Problem 4

Does boiling break water into H and O atoms?
Answer and explanation

No. Ordinary boiling primarily overcomes intermolecular attractions; the molecules remain H₂O.

Response criteria

  • State a scientifically accurate conclusion.
  • Show the calculation or mechanism that supports it.
  • Include units, conditions, or limits where relevant.

Problem 5

Find heat for 20 g material, c=2 J/(g·°C), warmed by 15°C. Show the reasoning, not just the conclusion.
Hints

Do not apply mcΔT alone to a phase-change plateau.

Answer and explanation

Q=20×2×15=600 J.

Problem 6

A sample melts while heating continues. What must a full energy calculation include?
Hints

State what the supplied observations or conditions establish, and separate that from any assumption.

Answer and explanation

Phase-change energy mL plus any separate warming before or after, with each segment counted once.

Problem 7

Latent energy changes phase fraction at the stated transitionLatent energy changes phase fraction at the stated transitionqphase = mL10.0 g ice × 334 J/g = 3340 JTemperature can remain near 0°C while melting.L depends on the substance, transition and pressure.
Original rounded water fusion example; it assumes the starting ice is already at the transition temperature and does not include container or environmental losses.
Interpret the supplied visual. Which sign describes heat for the sample during freezing if melting the same amount requires +3340 J?
Answer and explanation

Approximately −3340 J for the reverse transition under the corresponding conditions.

A specific latent energy L gives energy per mass for a particular phase change under specified conditions. Near ordinary-pressure melting, water’s fusion value is about 334 J/g. Melting ten grams of ice at its transition therefore needs about 3,340 J even while temperature is nearly constant. Vaporization has a different value, and reverse transitions have the opposite system heat sign. The energy concerns the full phase arrangement, not ordinary cleavage of every O–H covalent bond in the molecules.

Approximately −3340 J for the reverse transition under the corresponding conditions.

Response criteria

  • Interpret labels, structures, axes, units and directions correctly.
  • Explain the chemistry relationship or mechanism.
  • Respect stated assumptions and distinguish observation from inference.

Problem 8

For 20.0 g ice already at 0°C, calculate energy to melt it and warm the liquid to 10.0°C. Use Lf=334 J/g and c=4.18 J/(g·°C), neglecting apparatus/losses.
Answer and explanation

Melting: 20.0×334=6680 J. Warming: 20.0×4.18×10.0=836 J. Total=7516 J≈7.52 kJ. The sample receives positive heat under the stated boundary.

Melting: 20.0×334=6680 J. Warming: 20.0×4.18×10.0=836 J. Total=7516 J≈7.52 kJ. The sample receives positive heat under the stated boundary.

Response criteria

  • Use the stated measurements or conditions, with correct units.
  • Connect the result to the chemical mechanism or evidence relationship.
  • Identify the assumption, model limit or further evidence requested.

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