2. Thermal physics
- Syllabus
- 0625–2026–2027
- Section
- 2
- Level
- —
A state of matter can be distinguished by whether it keeps its own shape, keeps its own volume and can be compressed easily.
| State | Shape | Volume | Compression and flow |
|---|---|---|---|
| solid | fixed shape | fixed volume | difficult to compress; does not flow |
| liquid | takes the shape of the part of its container it occupies | fixed volume | difficult to compress; flows |
| gas | no fixed shape; spreads to fill its container | no fixed volume; expands to fill the container | easily compressed; flows |
If a sample takes its container's shape, it could be a liquid or a gas. Decide between them by asking whether it keeps a fixed volume: a liquid does, while a gas fills all available space.
Shape alone is not enough to distinguish a liquid from a gas. This card describes observable bulk properties only; particle arrangement, separation and motion belong to the next Topic.
A change of state changes whether a substance is solid, liquid or gas. Name the process from its starting state and finishing state.
| From | To | Name | Energy direction |
|---|---|---|---|
| solid | liquid | melting | energy is supplied |
| liquid | solid | freezing or solidification | energy is removed |
| liquid | gas | boiling or evaporation | energy is supplied |
| gas | liquid | condensation | energy is removed |
Learn the reverse pairs: melting ↔ freezing/solidification, and boiling/evaporation ↔ condensation. Water droplets forming outside a cold glass are produced by condensation of water vapour in the surrounding air; they do not leak through the glass.
Do not swap the direction: melting is solid to liquid, not liquid to solid; condensation is gas to liquid, not liquid to gas. Direct solid-to-gas and gas-to-solid changes are explicitly not required by this syllabus objective.
A simple particle model represents matter as tiny particles. To identify a state, compare three features: arrangement, average separation and motion.
| State | Arrangement and separation | Motion |
|---|---|---|
| solid | closely packed in an ordered pattern | vibrate about fixed positions |
| liquid | closely packed but irregular, with no fixed pattern | move around and slide past one another |
| gas | widely separated and randomly arranged | move rapidly and randomly in all directions |
In a simple diagram, use equal-sized circles. Draw a solid as close ordered rows, a liquid as close irregular circles, and a gas as circles spread far apart at random. The spaces are part of the model: a gas is easy to compress because its particles are far apart, whereas solids and liquids have little empty space between particles.
Do not draw larger particles when a substance changes state. The particle size and identity stay the same; it is their arrangement, separation and motion that change. The circles are schematic, so their exact number and drawn size are not measurements.
A higher temperature means that particles have a greater average kinetic energy and move faster on average; a lower temperature means less average kinetic energy and slower motion.
Heating transfers energy to the particles, so their average speed increases. Cooling removes energy, so their average speed decreases. In a sealed rigid container, heating changes speed but not the average separation, because the volume and number of particles stay fixed.
Absolute zero is the lowest possible temperature: −273 °C. At this temperature particles have their least kinetic energy. This is the syllabus statement to use when describing the lower limit of temperature.
Absolute zero is not 0 °C, and ‘least kinetic energy’ must not be replaced by ‘zero gravitational potential energy’. Do not claim that every particle has exactly the same speed: temperature describes average particle motion.
Gas pressure is produced because rapidly moving particles repeatedly collide with the surfaces of their container.
Each particle changes direction when it hits a surface. Across an enormous number of collisions, the surface experiences a continuous push. If a fixed amount of gas is heated in a rigid container, the particles move faster, hit the walls more often and make stronger impacts, so the pressure rises. Cooling reverses these changes and lowers the pressure.
The pressure does not rise because each particle expands or because new particles appear. Compare pressure changes only after stating what is held fixed; detailed force-per-area and momentum reasoning is developed in the Supplement card later in this Topic.
Microscopic particles suspended in a still liquid or gas can be seen moving continually in irregular, random directions. This observed motion is evidence for the kinetic particle model of matter.
| Stage | What it says |
|---|---|
| observation | a visible speck follows a jagged path with sudden changes of direction and unequal step lengths |
| evidence | the motion continues even though the suspension as a whole is still |
| conclusion | matter contains particles that are in continual random motion |
Record what is observed before explaining it: the path is random and jerky, not a smooth curve or motion in one common direction. The visible speck is a microscopic suspended particle; it is not an individual molecule of the liquid or gas.
Brownian motion is the continual random motion of microscopic particles in a suspension, caused by collisions with the much smaller particles of the surrounding liquid or gas.
The liquid or gas particles move rapidly and randomly. They strike every side of a suspended smoke particle or pollen grain, but the impacts are not perfectly balanced at each instant. The resulting unbalanced force changes the microscopic particle’s speed or direction. A new unequal set of impacts then changes its motion again, producing the observed irregular path.
The bright light makes the suspended particles visible; it does not drive their motion. Convection currents, collisions between the suspended particles, and the suspended particle’s own atoms are not the Brownian-motion mechanism described here.
The properties of a solid, liquid or gas result from the combined effects of particle separation, forces between particles and particle motion.
| State | Separation and forces | Motion | Resulting properties |
|---|---|---|---|
| solid | particles are close; attractive forces are strong | particles vibrate about fixed positions | fixed shape and volume; difficult to compress |
| liquid | particles are close; forces keep them together but not in fixed positions | particles move and slide past one another | fixed volume but no fixed shape; flows; difficult to compress |
| gas | particles are far apart; forces are negligible except during collisions | particles move rapidly and randomly | fills its container; no fixed volume; easy to compress |
‘Particle’ is a general model word. Depending on the substance, the relevant particles may be atoms, molecules, ions or electrons. Do not assume that every material is made of molecules.
No single feature explains every property. Close spacing helps explain low compressibility, while forces and freedom of motion distinguish a rigid solid from a flowing liquid. Strong forces alone do not mean that particles are motionless.
When a gas particle strikes and rebounds from a surface, its momentum changes. That change requires a force, and the particle exerts an equal force on the surface.
A huge number of impacts produces a total force on the wall. More collisions each second or a greater momentum change in each collision increases that total force. Gas pressure is the total normal force from these impacts divided by the area over which it acts.
p=AF
Here p is pressure, F is the total force perpendicular to the surface, and A is the surface area. For the same area, a larger collision force gives a larger pressure; for the same force, spreading it over a larger area gives a smaller pressure.
Pressure is not the same quantity as force. A correct particle explanation links collision and rebound → change of momentum → force on the surface → force per unit area.
In a Brownian-motion experiment, the visible microscopic particle and the invisible atoms or molecules of the surrounding fluid are different objects.
| Object | Relative scale and motion | Correct description |
|---|---|---|
| atom or molecule of the liquid or gas | much lighter, fast-moving and not seen individually in this experiment | collides with the microscopic particle and may rebound |
| microscopic smoke particle or pollen grain | much larger and heavier; visible as a speck through the microscope | is moved by the changing, unequal total effect of many molecular collisions |
For example, a fast nitrogen molecule can strike a stationary smoke particle: the smoke particle moves and the nitrogen molecule rebounds. Many such impacts from changing directions create the smoke particle’s irregular motion.
Say ‘smoke particle’ or ‘pollen grain’, not ‘smoke molecule’ or ‘pollen molecule’. Microscopic means small enough to require a microscope; it does not mean the same size as an atom or molecule.
For a fixed mass of gas, pressure changes when particle speed changes or when the same particles collide with the walls more or less frequently.
| Controlled change | Particle account | Pressure effect |
|---|---|---|
| temperature increases at constant volume | particles gain average kinetic energy, move faster, and make more frequent and harder collisions with the same walls | pressure increases |
| temperature decreases at constant volume | particles move more slowly, so collisions are less frequent and less forceful | pressure decreases |
| volume decreases at constant temperature | average speed stays the same, but particles cross a shorter distance and hit each unit area of wall more frequently | pressure increases |
| volume increases at constant temperature | average speed stays the same, but collisions with each unit area of wall become less frequent | pressure decreases |
Name the control before predicting the pressure. Constant volume isolates the effect of temperature on particle speed. Constant temperature isolates the effect of volume on collision frequency; the particles do not speed up merely because the gas is compressed slowly.
These comparisons require the same fixed mass of gas. If gas leaks in or out, or if temperature and volume both change, one simple comparison is not enough to predict the result without further information.
The kelvin and Celsius scales have equal-sized intervals but different zero points: 0 K corresponds to −273 °C.
T(K)=θ(∘C)+273
To convert °C to K, add 273. To convert K to °C, rearrange to θ=T−273.
Examples: 25∘C=25+273=298K. For nitrogen at 77K, θ=77−273=−196∘C.
Write K, not °K: kelvin has no degree sign. A temperature can be negative on the Celsius scale while remaining positive in kelvin; for example, −196 °C is 77 K.
For a fixed mass of gas at constant temperature, pressure and volume are inversely proportional: increasing one decreases the other so that their product stays constant.
pV=constantsop1V1=p2V2
A gas at 120kPa occupies 50cm3 and is compressed at constant temperature to 30cm3. Then p2=(120×50)/30=200kPa. The pressure rises because the volume falls.
On a graph of p against V, the relationship is a decreasing curved line: doubling V halves p, and halving V doubles p. The curve becomes less steep as volume increases and does not meet either axis. A graph of p against 1/V is a straight line through the origin.
Use one consistent volume unit on both sides and one consistent pressure unit on both sides; matching units cancel in the ratio. Do not use pV=constant if the gas mass or temperature changes.
At constant pressure, most solids, liquids and gases expand when heated and contract when cooled: their dimensions or volume change with temperature.
| State | When heated at constant pressure | When cooled |
|---|---|---|
| solid | length, area and volume increase slightly; any hole in the solid also becomes larger | length, area, volume and holes become smaller |
| liquid | volume increases, usually more than the containing solid | volume decreases |
| gas | volume increases substantially if its boundary can move | volume decreases |
Expansion does not add matter: the mass stays constant. Because the same mass occupies a larger volume, density decreases on heating; contraction at constant mass increases density.
The particles themselves do not get larger. ‘Gas expands when heated’ here assumes constant pressure and space for the gas boundary to move. In a sealed rigid container the volume cannot expand, so heating raises the pressure instead.
Thermal expansion is useful when a changing size produces a measurement or movement, but unwanted expansion must be allowed for so structures do not bend, buckle or crack.
| Situation | Expansion or contraction | Design response or useful effect |
|---|---|---|
| railway tracks and bridges | long sections expand in hot weather | leave expansion gaps or joints so the sections can lengthen without buckling |
| overhead cables | metal contracts in cold weather | install the cable with slack so contraction does not create a dangerously large tension |
| tight metal lid on a glass jar | for the same warming, the metal lid expands more than the glass neck | the lid opening becomes relatively larger, making the lid easier to remove |
| liquid-in-glass thermometer | the liquid expands more than the glass bulb | liquid rises along a narrow uniform capillary; a narrower tube gives a larger rise per degree |
| thermostat with a bimetallic strip | its two bonded metals expand by different amounts | the strip bends and can open or close an electrical contact |
For each example, identify what changes temperature, which part expands or contracts, and what would happen without the design feature. A gap is useful because the material expands into it; the gap itself is not the expanding object.
Do not explain every heating effect as expansion: melting and simply becoming hotter are different processes. The application must depend on a change in dimensions or volume.
For the same temperature rise at constant pressure, the usual order of volume expansion is gas > liquid > solid.
| State | Particle arrangement and forces | Effect of heating | Relative expansion |
|---|---|---|---|
| solid | particles are close and held strongly in fixed positions | vibrations become more energetic and average separation increases only slightly | least |
| liquid | particles are close but can move past one another; attractions are weaker than in a solid | faster motion produces a larger increase in average separation | intermediate |
| gas | particles are already far apart and attractions are negligible | faster particles spread much farther apart while the gas volume grows to keep pressure constant | greatest |
Heating increases particle kinetic energy. The size change comes from an increase in average separation, not from particles swelling. Stronger constraints in a solid resist separation most; the weakly constrained gas changes volume most.
Compare equal temperature rises under the same constant-pressure condition. The statement is an order of magnitudes, not a claim that every solid, liquid or gas has one identical expansion value.
When an object's temperature rises, its internal energy increases. Internal energy is energy stored by all the particles in the object; temperature is a measurement, not an energy store.
The statement describes a change in one object: compare it before and after heating. Energy transferred to the object raises its internal energy, and a temperature rise is evidence of that increase.
Temperature and internal energy are not the same quantity. A large amount of cooler material can have more internal energy than a small hot object, so temperature alone does not give an object's total internal energy.
An increase in temperature means an increase in the average kinetic energy of all the particles in the object.
| State | What the greater average kinetic energy looks like |
|---|---|
| solid | particles vibrate more energetically about their fixed positions |
| liquid | particles move around one another faster on average |
| gas | particles travel faster on average between collisions |
‘Average’ matters: particles do not all have identical kinetic energy or move at one identical speed. The distribution changes so that the mean kinetic energy of the whole collection is greater.
Do not say that heating makes particles themselves larger. The temperature change is explained by their motion and kinetic energy, not by a change in particle size.
Specific heat capacity, c, is the energy required per unit mass of a substance for a unit increase in temperature. Its unit is J/(kg °C), equivalently J kg⁻¹ °C⁻¹.
c=\frac{\Delta E}{m\Delta T}\qquad\text{and therefore}\qquad\Delta E=mc\Delta T
Here ΔE is the increase in internal energy in joules, m is mass in kilograms, and ΔT is the temperature rise in °C. A temperature interval has the same numerical size in °C and K.
Example: a 0.80 kg aluminium block receives 18 000 J and warms by 25 °C.
c=0.80×2518000=900 J/(kg °C)
The substitution uses the temperature change, not the final temperature.
A larger c means more energy is needed to produce the same temperature rise in the same mass. It does not mean the substance automatically heats faster; with the same energy input, a larger c gives a smaller temperature rise.
Measure the sample's mass m, the electrical energy supplied ΔE, and its temperature rise ΔT, then calculate c=ΔE/(mΔT). If heater power P is known, ΔE=Pt; otherwise use ΔE=VIt.
| Feature | Solid block | Liquid |
|---|---|---|
| sample mass | measure the block on a balance | measure filled container minus empty container |
| heater and thermometer | place them in snug holes with good thermal contact | immerse both in the liquid; keep them clear of the container wall |
| limiting heat transfer | wrap the block in insulation | use an insulated container and lid |
| uniform temperature | allow the block to conduct energy through it | stir the liquid gently while heating |
Insulate the sample, use a lid for a liquid, ensure good heater contact in a solid, and stir a liquid. Some electrical energy warms the heater, thermometer and container or escapes to the surroundings. Treating all supplied energy as energy gained by the sample makes the calculated c too large.
During melting and boiling, a substance absorbs energy while its temperature remains constant until the change of state is complete.
| Change | Energy transfer | What changes while temperature is constant |
|---|---|---|
| melting: solid → liquid | energy enters the substance | particles become less strongly held and can move past one another |
| boiling: liquid → gas | energy enters the substance | particles overcome attractions and separate widely as gas |
Temperature depends on average particle kinetic energy. During the change of state, the input increases particle separation and potential energy rather than average kinetic energy, so the temperature does not rise. After the change is complete, further energy input can raise the temperature again.
A flat section on a heating curve does not mean that no energy is entering. It means energy is changing the state instead of increasing the temperature. This course objective is qualitative; no specific-latent-heat calculation is required.
At standard atmospheric pressure, pure water melts and freezes at 0 °C, and boils and condenses at 100 °C.
| Temperature | Processes in opposite directions | Coexisting states during the change |
|---|---|---|
| 0 °C | melting ↔ freezing | ice and liquid water |
| 100 °C | boiling ↔ condensation | liquid water and water vapour |
These values assume standard atmospheric pressure and pure water. The numbers are phase-change temperatures, not the lowest and highest temperatures a thermometer can read.
Condensation changes a gas to a liquid; solidification changes a liquid to a solid. In both changes, the substance releases energy as attractions constrain the particles more strongly.
| Change | Particle account |
|---|---|
| condensation: gas → liquid | particles come much closer together; attractions keep them close while they still move randomly past one another |
| solidification: liquid → solid | particles become held in fixed positions in an ordered, closely packed arrangement; they continue to vibrate |
At the phase-change temperature, average kinetic energy and temperature remain constant while potential energy decreases and energy is transferred out. Particles do not disappear, shrink or stop moving.
Evaporation occurs when more-energetic particles at the surface of a liquid have enough energy to overcome attractions and escape into the gas above the liquid.
Liquid particles have a range of kinetic energies. At any moment, some surface particles are energetic enough to leave, even when the liquid is below its boiling point. Particles deeper in the liquid cannot escape directly through the surface.
Evaporation is not a stream of bubbles through the liquid. It is a surface process and can occur at many temperatures, not only at the boiling point.
Evaporation causes the temperature of the remaining liquid to decrease.
More-energetic particles are more likely to escape → they carry away more than the average kinetic energy → the particles left behind have a lower average kinetic energy → the liquid's temperature falls.
Cooling is about the average energy of the particles that remain. It is not because moving air directly slows every particle in the liquid.
Boiling and evaporation both change liquid to gas, but they occur in different ways.
| Feature | Boiling | Evaporation |
|---|---|---|
| where | throughout the liquid | only at the surface |
| temperature | at the boiling point for the stated pressure | can occur at many temperatures |
| visible behaviour | vapour bubbles form within the liquid and rise | no vapour bubbles form throughout the liquid |
| effect during the process | with continued energy input, temperature stays constant while boiling | preferential escape often cools the remaining liquid |
Steam-like mist above a liquid is not evidence that evaporation occurs throughout it. The key test is whether vapour bubbles form within the body of the liquid.
Evaporation is faster when the liquid is warmer, when its exposed surface area is larger, and when air moves more quickly over the surface.
| Change | Effect on rate | Particle reason |
|---|---|---|
| raise temperature | increases | a larger fraction of particles has enough energy to escape |
| increase exposed surface area | increases | more particles are at the surface and able to escape at once |
| increase air movement | increases | vapour particles are carried away, so fewer return to the liquid |
A wide dish evaporates faster than a narrow container holding the same volume at the same temperature. Wet clothes dry fastest when spread out in warm, moving air.
Moving air does not speed evaporation by adding kinetic energy directly to the liquid. Its main role is to remove vapour from above the surface.
An object in contact with an evaporating liquid cools because energy transfers from the object to the liquid and is carried away as particles escape.
Evaporation removes energetic liquid particles → the liquid needs energy to continue evaporating → energy transfers from the warmer object into the liquid → the object's internal energy and temperature decrease.
Sweat cools skin, a volatile liquid used on skin feels cold, and a wet cloth can cool a container. Faster evaporation usually increases the cooling rate because energy is removed from the object more quickly.
Do not stop at ‘the liquid cools’. To explain cooling of the object, state the energy-transfer direction: from the object into the evaporating liquid and then away with the vapour.
A good thermal conductor transfers energy quickly through itself; a poor conductor, or thermal insulator, transfers energy slowly.
| Method | Set-up and observation | Conclusion |
|---|---|---|
| wax-pin comparison | use rods of equal length and diameter; attach identical pins with equal wax blobs at the same distance from one end; heat the ends equally and record when each pin falls | the rod whose wax melts first is the better conductor |
| temperature comparison | place equal lengths of different rods equally deep in hot water; measure temperature at points the same distance from the water at equal times | the rod whose measured point warms faster is the better conductor |
Keep rod dimensions, distance from the heated end, initial temperature, heating time or water temperature, wax amount and thermometer position the same. Repeat readings so the comparison depends on material rather than geometry or heating.
Feeling metal and plastic at the same room temperature shows how quickly they transfer energy to or from the hand, not that the metal began colder.
Thermal conduction in every solid occurs through lattice vibrations. Metals have an additional, faster route: mobile delocalised electrons.
| Solid | How energy moves from hotter to cooler regions |
|---|---|
| all solids | particles at the hot end vibrate more energetically and transfer energy to neighbouring lattice particles, so the vibration spreads through the solid |
| metals | delocalised electrons gain energy in the hot region, move through the lattice and transfer energy in collisions with ions; lattice vibration also occurs |
The atoms, molecules or ions remain around fixed lattice positions; they do not travel from the hot end to the cold end. Energy is passed through the solid down the temperature difference.
Positive ions do not move freely through a metal. Metals usually conduct better than non-metals because mobile electrons provide an extra energy-transfer route, not because metal atoms migrate along the object.
Gases and most liquids are poor thermal conductors because their particles are not held in a closely connected, fixed lattice.
| Material | Particle arrangement | Consequence for conduction |
|---|---|---|
| non-metal solid | particles are close in a lattice | vibrations pass energy repeatedly to neighbouring particles |
| liquid | particles are close but not fixed in a lattice | collisions can transfer energy, but there is no continuous lattice-vibration pathway |
| gas | particles are far apart | collisions are much less frequent, so conduction is especially slow |
Poor conduction does not mean no energy transfer. Liquids and gases can still transfer energy slowly by particle collisions, and bulk movement may also transfer energy by convection; this card is comparing conduction only.
Solids do not fall into only two absolute groups. Many solids conduct thermal energy better than thermal insulators but less well than good thermal conductors.
| Position on the conduction scale | Behaviour for the same shape and temperature difference |
|---|---|
| good thermal conductor | transfers energy rapidly |
| intermediate solid | transfers energy at a moderate rate |
| thermal insulator | transfers energy slowly |
‘Conductor’ and ‘insulator’ are comparative descriptions. Choose a material by comparing transfer rates under the same conditions; a solid called an insulator still conducts some energy.
Do not infer that every non-metal is equally insulating or that every metal has one identical conductivity. Material, thickness, area and temperature difference all matter in a real comparison.
Convection is thermal energy transfer by the bulk movement of a fluid. It is an important transfer method in liquids and gases because their particles can move from place to place.
| Medium | Can convection occur? | Reason |
|---|---|---|
| liquid | yes | the liquid can flow and carry internal energy |
| gas | yes | the gas can flow and carry internal energy |
| solid | no | its particles do not move through the solid as a bulk flow |
| vacuum | no | there is no matter to move |
Convection circulates water heated in a pan and air heated in a room. The fluid itself moves, carrying energy from one region to another.
Do not say ‘heat rises’. Warmer, less-dense fluid may rise, while cooler, denser fluid moves down to replace it; thermal energy is carried with the moving fluid.
A convection current is a continuous circulation caused by density differences within a liquid or gas.
| Step | What happens |
|---|---|
| 1 | a region of fluid is heated, expands and becomes less dense |
| 2 | the warmer, less-dense fluid rises |
| 3 | cooler, denser fluid moves down to replace it |
| 4 | continued heating and cooling maintain a circulating current that transfers energy |
| Fluid | Demonstration | Observation and conclusion |
|---|---|---|
| liquid | place a small coloured tracer near the bottom at one side of a beaker of water and heat gently below it | the coloured water rises above the heater, moves across the top and descends on the cooler side, showing a convection current |
| gas | use a convection box with two chimneys; warm the air below one chimney and introduce smoke at the other | smoke is drawn down the cool chimney, crosses the box and rises out above the heater, tracing the air current |
Cooling can drive the same cycle in reverse locally: water beside ice cools, becomes denser and sinks; warmer water rises to replace it. The result is still a convection current.
Rising and sinking are consequences of density differences, not separate transfer methods. A complete explanation links temperature change to density change, fluid motion, replacement and circulation.
Thermal radiation is infrared radiation, a region of the electromagnetic spectrum. Every object emits infrared radiation.
| Claim | Meaning |
|---|---|
| type of radiation | infrared electromagnetic radiation |
| emitters | all objects, not only visibly glowing objects |
| transfer | an object can emit infrared that another object absorbs |
Visible light may also be emitted by a very hot object, but the thermal-radiation region named in this syllabus is infrared.
Infrared radiation does not require a material medium. As electromagnetic radiation, it can transfer thermal energy through a vacuum.
| Process | Needs matter between source and receiver? | Can cross a vacuum? |
|---|---|---|
| conduction | yes | no |
| convection | yes, a moving fluid | no |
| radiation | no | yes |
Energy from the Sun and stars reaches Earth across space by radiation. The receiving surface warms when it absorbs that radiation.
A vacuum does not block radiation. It prevents conduction and convection between separated objects because those processes require matter.
Surface colour and texture affect how strongly infrared radiation is emitted, absorbed and reflected.
| Surface feature | Absorption | Emission | Reflection |
|---|---|---|---|
| black | better | better | poorer |
| white | poorer | poorer | better |
| dull | better | better | poorer |
| shiny | poorer | poorer | better |
For the strongest contrast, dull black surfaces are good absorbers and emitters, while shiny white or polished silver surfaces are good reflectors and poor absorbers and emitters. Compare otherwise identical surfaces at the same temperature and area.
Do not describe a surface as a ‘conductor of radiation’. Conduction is a different transfer process; surfaces absorb, emit or reflect infrared radiation.
For an object in a steady state with no change of state, temperature remains constant when the rate at which it receives energy equals the rate at which it transfers energy away.
| Energy transfer in | Energy transfer out | Temperature result |
|---|---|---|
| equal rates | equal rates | constant |
Energy can continue to enter and leave the object. Constant temperature means no net change in its internal energy because the two rates balance.
Thermal balance is not the same as zero energy transfer. A heater may supply energy continuously while the object transfers energy away at the same rate. During melting or boiling, temperature can also remain constant while internal energy changes; that phase-change case is treated separately.
When no change of state occurs, temperature changes if the rate of energy transfer into an object differs from the rate of transfer out.
| Comparison of rates | Internal energy | Temperature |
|---|---|---|
| input rate greater than output rate | increases | rises |
| input rate equal to output rate | constant | remains constant |
| input rate less than output rate | decreases | falls |
As a hot object cools, its temperature difference from the surroundings becomes smaller, so its cooling rate usually decreases. It approaches the surroundings' temperature as the rates move towards balance.
Compare rates, not just total amounts already transferred. With no phase change, the sign of input rate minus output rate determines whether temperature is rising or falling at that moment.
Earth's average surface temperature is controlled by the balance between incoming radiation absorbed from the Sun and outgoing infrared radiation emitted towards space.
| Planetary balance | Temperature tendency |
|---|---|
| absorbed incoming rate greater than outgoing rate | average temperature rises |
| absorbed incoming rate equal to outgoing rate | average temperature is steady |
| absorbed incoming rate less than outgoing rate | average temperature falls |
An increase in greenhouse gases can reduce the rate at which outgoing infrared escapes to space. While absorbed incoming radiation exceeds outgoing radiation, the surface warms until a new balance may be reached.
Incoming sunlight and outgoing infrared are different parts of Earth's energy budget. A temperature rise indicates a rate imbalance, not that Earth has stopped emitting radiation.
A good emitter produces a larger infrared detector response than a poor emitter when surface temperature, area and distance are the same.
| Stage | What to do |
|---|---|
| set up | use equal-area dull black and shiny or white surfaces on the same hot container, or identical containers with equal hot-water volumes and temperatures |
| measure | place the same infrared detector or matched black-bulb thermometers at equal perpendicular distances; record readings at equal times |
| result | the dull black surface gives the larger detector response or faster thermometer rise |
| conclusion | dull black is the better emitter; shiny or white is the poorer emitter |
Control surface area, surface temperature, detector distance and angle, water volume and initial temperature, container dimensions and observation time.
A faster fall in a hot container's temperature can also indicate stronger emission, but only when other energy-transfer paths and all comparison variables are controlled.
A good absorber produces a faster temperature rise than a poor absorber when both receive the same infrared radiation.
| Stage | What to do |
|---|---|
| set up | use identical dull black and shiny or white cans containing equal volumes of water at the same initial temperature |
| expose | place both cans at equal distance and orientation from the same radiant heater; switch it on for the same time |
| measure | record both water temperatures at equal time intervals |
| result and conclusion | the water in the dull black can warms faster, so dull black is the better absorber |
Control can material and dimensions, exposed area, water mass, initial temperature, heater power, distance, angle and heating time.
This compares absorption of incoming radiation. Do not infer the result from thermal conductivity of the can, and do not change both surface and geometry at once.
For otherwise comparable objects, infrared emission increases with surface temperature and with emitting surface area.
| Change while other factors stay fixed | Rate of infrared emission |
|---|---|
| higher surface temperature | greater |
| lower surface temperature | smaller |
| larger emitting surface area | greater total rate |
| smaller emitting surface area | smaller total rate |
Compare one factor at a time: use the same surface finish when testing temperature or area. Surface colour and texture also affect emission, as covered separately.
A larger area increases the total emitted power; it does not mean each square centimetre emits more when temperature and surface finish are unchanged.
Everyday heating devices use material choice and fluid circulation to direct thermal energy where it is useful and reduce transfer where it is unsafe.
| Pan feature or process | Thermal explanation |
|---|---|
| metal base | a good conductor transfers energy rapidly from the heater into the pan and contents |
| plastic or wooden handle | a poor conductor reduces transfer to the hand |
| water in the pan | warmer, less-dense water rises and cooler, denser water sinks, so convection circulates energy through the liquid |
| Step in room heating | Explanation |
|---|---|
| air near the heater warms | its density decreases |
| warm air rises | cooler, denser air moves down to replace it |
| circulation continues | the convection current transfers energy around the room |
Name the process at each stage. Conduction transfers energy through the solid pan; convection is the bulk circulation of water or air. Saying only ‘heat rises’ does not explain room heating.
Complex thermal systems can involve conduction through solids, convection by moving fluids and infrared radiation across space at the same time.
| Process | Role in a wood or coal fire |
|---|---|
| conduction | energy spreads through touching parts and within solid fuel, helping nearby material heat up |
| convection | hot gases rise and cooler oxygen-containing air is drawn towards the fire; rising gases carry energy upward |
| radiation | flames and hot fuel emit infrared that warms surroundings and can preheat nearby fuel |
| Process | Role in cooling the engine |
|---|---|
| conduction | energy passes from engine metal to coolant and from hot coolant through radiator tubes into metal fins |
| convection | pumped coolant carries energy to the radiator; moving air carries energy away from the tubes and fins |
| radiation | hot radiator surfaces also emit infrared to the surroundings |
A radiator uses metal tubes and many fins: good conduction moves energy to the surface, while the large area and airflow increase transfer to the air. Radiation occurs, but forced convection is usually the main external cooling route.
The name ‘radiator’ does not mean a car radiator cools mainly by radiation. Identify each path from the material that carries energy: solid metal, moving coolant or air, or infrared radiation.