Thermodynamics (Topic 9)Heating and internal energy (Topic 9A)

Heating and internal energy (Topic 9A)

Specific heat capacity, latent heat, internal energy, absolute zero and molecular kinetic energy in Edexcel A-level Physics.
14 min

The specific heat capacity of a substance is defined as:

THE SPECIFIC HEAT CAPACITY. The amount of thermal energy required to raise the temperature of 1 kg of the substance by 1 °C. Thermometer showing +1 °C. Heater connected to an Aluminium block labeled 1 kg. Power supply with controls.

Specific heat capacity is a measure of how much a material resists changes in temperature.

Specific heat capacity is expressed in units of (joules per kilogram per Kelvin) or (joules per kilogram per degree Celsius) and is denoted by the symbol

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The relationship between energy, mass, specific heat capacity, and temperature change is given by:

Where:

  • is the thermal energy transferred (in J),
  • is the mass of the substance (in kg),
  • is the specific heat capacity (in or , and
  • is the temperature change (in K or \)

The change in a substance’s temperature depends on:

  • Mass: A larger mass requires more energy to achieve the same temperature change because there is more material to be heated.
  • Thermal energy: A greater temperature change requires a larger amount of thermal energy.
  • Specific heat capacity: Substances with higher specific heat capacities require more energy to raise their temperature.
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Substances with low specific heat capacity:

  • Heat up and cool down quickly.
  • Examples: Metals such as copper and lead have low specific heat capacities, making them efficient conductors of heat.
  • These materials are ideal for applications such as cooking utensils, where rapid heat transfer is crucial.

Substances with high specific heat capacity:

  • Heat up and cool down slowly.
  • Examples: Water has a very high specific heat capacity, making it excellent for storing and transporting heat.
  • High value substances are useful in systems such as radiators or thermal insulators, where slow temperature changes are desirable.
A table displaying materials and their specific heat capacity in joules per kilogram per degree Celsius. The materials listed are Copper (390), Aluminium (910), Water (4200), Air, dry (sea level) (1005), Brick (840), Iron (449), Wood (1300–2400), and Porcelain (1085).

Metals such as copper and lead are excellent heat conductors due to the presence of free electrons, which efficiently carry thermal energy. This ability to transfer heat quickly explains their low specific heat capacities.

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When calculating specific heat capacity or related energy transfers, it is crucial to use the temperature change not just the final temperature.

Do

Calculate the temperature change using:

This ensures you get the correct sign for the temperature change:

  • If the temperature increases, energy is absorbed (positive
  • If the temperature decreases, energy is released (negative

Don't
  • Confuse the final temperature with the temperature change
  • Mix temperature units. Ensure all temperatures are in the same unit (e.g. or K). Note that temperature changes are the same in both units, so does not depend on converting between and K.
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Some practical applications of specific heat capacity:

Heating systems: Water is used in central heating systems. Its high specific heat capacity allows it to store a large amount of heat. Cooking: Metals like aluminium and copper, with low specific heat capacities, are ideal for making pans and pots, as they heat up quickly and transfer heat efficiently. Thermal insulators: Materials with high specific heat capacities are used to maintain stable temperatures. For example, ceramics are used for coffee mugs, allowing you to hold a hot drink without burning yourself. Earth’s climate: Water's high specific heat capacity plays a crucial role in regulating Earth's climate, as it absorbs and releases large amounts of heat in oceans and lakes.
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Question walkthrough

Specific Heat Capacity with Energy Losses

Calculate the specific heat capacity of a metal block heated by an electric heater, accounting for a percentage of the supplied energy lost to the surroundings.

Question walkthrough

Method of Mixtures: Copper and Water

Use conservation of energy to find the specific heat capacity of copper from the equilibrium temperature reached when a hot copper block is placed into water.

Energy is required to change the state of a substance.

When a change of state occurs, energy is supplied to overcome intermolecular forces, not to increase temperature – the temperature remains constant.

The diagram below illustrates the key state changes to remember:

A diagram illustrating the states of matter: Solids, Liquids, and Gases. Arrows indicate processes: Melting and Freezing between Solids and Liquids; Evaporation/boiling and Condensation between Liquids and Gases; Sublimation from Solids to Gases; and Deposition from Gases to Solids, highlighted in red.

It is useful to note that there is an additional state of change called deposition, where a gas changes directly into a solid without passing through a liquid phase. However, knowledge of this change of state is not required for your exams.

An example of deposition is water vapour in the air depositing as a solid, crystalline frost on a window in cold conditions, bypassing the liquid water state.

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The energy required to change the state of a substance without altering its temperature is called latent heat. It is a property that varies depending on the material and state change.

The latent heat of fusion is the amount of energy required to change 1 kg of a substance from a solid to a liquid without a change in temperature.

Energy is required to overcome some of the intermolecular forces holding the solid together, allowing the particles to move more freely in the liquid state.

  • Melting: Energy is absorbed to break some intermolecular bonds, allowing the solid to turn into a liquid.
  • Freezing: The same amount of energy is released when a liquid solidifies, as bonds reform.
  • For water: The latent heat of fusion is , meaning 330 kJ is needed to melt 1 kg of ice at
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The latent heat of vaporisation is the energy required to change of a substance from a liquid to a gas without a change in temperature.

Energy is required to completely break the intermolecular forces, allowing particles to move freely as a gas.

  • Boiling/evaporation: Energy is absorbed to completely separate molecules.
  • Condensation: The same amount of energy is released when a gas turns back into a liquid.
  • For water: The latent heat of vaporisation is , meaning is needed to turn 1 kg of water into steam at This means evaporating of water requires about 7 times more energy than melting the same amount of ice.
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The energy required for a substance to change state can be calculated using the formula:

Where:

  • is the thermal energy supplied or released (J),
  • m is the mass of the substance (kg), and
  • L is the specific latent heat .

Substances with low latent heat values change state more easily, requiring less energy. Substances with low latent heat can be used for precise temperature control.

Substances with high latent heat values are more stable during state changes, making them useful in thermal storage or cooling applications. Water’s high is why sweating effectively cools the body.

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Heating curves show how the temperature of a substance changes as heat is supplied.

Heating curves demonstrate how temperature remains constant during state changes.

A graph showing the relationship between Temperature and Heat supplied, with three sections labeled: Solids, Liquids, and Gases. The graph includes arrows indicating particle movement in each state. It also features the phrases 'Latent heat of fusion' in purple and 'Latent heat of vaporisation' in green.

When a substance is melting or boiling, all of the energy supplied is being used to change its state, not to raise its temperature, so the temperature remains constant.

While the temperature is constant, the latent heat equation applies:

allowing the latent heat to be determined.

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Question walkthrough

Specific Latent Heats of Fusion and Vaporisation

Calculate specific latent heats of fusion and vaporisation from electrical heating data, and explain why vaporisation requires much more energy than fusion.

The specific latent heat of a substance can be determined by measuring:

  • The energy supplied to the substance
  • The mass of the substance that changes state.

Then rearranging the formula below to make the subject:

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Method for measuring the specific latent heat of fusion of ice:

  1. Place ice cubes in a funnel with filter paper, above a beaker, to isolate the melted water from the ice block.
  2. Use two beakers:
    1. Beaker A collects water from ice melted by the immersion heater and by the surrounding air.
    2. Beaker B collects water from naturally melting ice exclusively.
  3. Heat the ice with an immersion heater and ensure the electrical circuit is set up for accurate ammeter and voltmeter readings.
  4. Record the current voltage and heating time
  5. After a set time, measure the mass of water in both beakers with an electronic balance.
  6. Isolate the mass melted by the heater alone by calculating the difference in mass readings.
  7. Calculate the specific latent heat fusion of ice:

A diagram showing a power supply connected to an immersion heater. There are two beakers labeled Beaker A and Beaker B on electronic balances displaying weights of 52 and 16, respectively. Ice cubes are shown being filtered through filter paper into Beaker B, while voltmeter (in parallel across heater) and ammeter (in series with heater) are also depicted.

Sources of error:

  • Filter paper absorbs water: Use non-absorbent material if possible.
  • Incomplete thermal equilibrium: If ice is not at some energy is used to raise its temperature before melting begins.
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Method for measuring the specific latent heat of vaporisation of water:

  1. Use a double-walled glass vessel to reduce heat loss and focus energy on vaporisation.
  2. A condenser ensures the vapour is collected efficiently for mass measurements.
  3. Collect condensed vapour: Ensure that the entire vapour from the liquid is condensed and collected to accurately measure its mass.
An illustration showing a laboratory setup with labeled components: X, Y, Outer flask, Condenser, Cold water, Collecting flask, Heater, Liquid, Inner flask, Vapour, and Vapour to condenser.

Sources of error:

  • Heat loss in the condenser: If vapour escapes before condensing, the mass of collected water will be underestimated, resulting in a higher latent heat value
  • Energy loss to surroundings: Not all energy from the heater goes into vaporisation; some heats the environment, causing overestimation of
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Potential sources of error common to both the method for measuring the specific latent heat of fusion of ice and the method for measuring the specific latent heat of vaporisation of water are listed below.

  • Heat loss to the surroundings is a major source of error in both and measurements. To minimise it:
    • Use insulating materials for beakers and vessels
    • Limit the system’s exposure to open air
    • Conduct the experiment in a draught-free environment.
  • Ensure the mass balance is zeroed correctly before weighing substances or collecting water.
  • Measure voltage and current periodically and calculate an average to account for fluctuations in the power supply.
  • Always monitor the temperature closely to ensure no unintended heating occurs beyond the state change point.
    • Latent heat of fusion: Ice remains at while it melts. Ensure the thermometer shows no temperature rise during the process.
    • Latent heat of vaporisation: water remains at (at standard pressure) while it boils.

After calculating or compare the value with known values for the substance (e.g. water has values of and to assess the accuracy of your experiment. Large deviations could indicate heat loss or instrument errors.

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The three main phases of matter are solids, liquids, and gases.

The solid phase is the most ordered, followed by the liquid phase, and the gas phase is the least ordered.

Solids have the following properties:

  • The spacing between the particles is small.
  • The particles are ordered, arranged in a regular structure.
  • The particles vibrate about fixed positions.
A grid of blue circles representing particles in a solid state, with the label 'Solid' at the bottom.
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The three main phases of matter are solids, liquids, and gases.

The solid phase is the most ordered, followed by the liquid phase, and the gas phase is the least ordered.

Solids have the following properties:

  • The spacing between the particles is small.
  • The particles are ordered, arranged in a regular structure.
  • The particles vibrate about fixed positions.
A grid of blue circles representing particles in a solid state, with the label 'Solid' at the bottom.
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Gases have the following properties:

  • The spacing between the particles is large.
  • The particles move at high speeds.
An illustration showing blue spheres representing gas molecules, with wavy lines indicating movement. The word 'Gases' is displayed at the bottom.
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The kinetic model explains the phases of matter in terms of particle motion.

In a solid, particles experience strong electrostatic forces, so they can only vibrate about fixed positions and cannot move freely.

  1. When a solid is heated, the particles gain kinetic energy and vibrate more strongly.
  2. Once they have enough energy to overcome some of the attractive forces, the solid melts and becomes a liquid.
An illustration showing the process of melting. On the left, a grid of blue circles labeled 'Solid' represents a solid state. On the right, a more spaced arrangement of blue circles labeled 'Liquid' represents a liquid state. An arrow points from the solid to the liquid, indicating the transition.
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In a liquid, particles experience weaker electrostatic forces than in a solid, allowing them to move past each other while remaining close together.

Liquid particles, therefore, have greater kinetic energy than solid particles.

  1. When a liquid is heated, the particles gain kinetic energy and move faster.
  2. Evaporation occurs when particles on the surface gain sufficient energy to overcome intermolecular forces and escape, resulting in the formation of a gas.
A diagram illustrating the process of Evaporation/Boiling. On the left, a cluster of blue spheres represents a Liquid, while on the right, scattered blue spheres depict a Gas. An arrow indicates the transition from Liquid to Gas.

It is important to note that evaporation is distinct from boiling:

  • Evaporation is a surface phenomenon that occurs at any temperature, where high-energy particles escape into a gas.
  • Boiling happens at a fixed temperature throughout the liquid, as particles gain enough energy to form gas bubbles.
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In a gas, particles experience negligible intermolecular forces, except during collisions. As a result, gas particles move freely in random directions.

Gas particles have greater kinetic energy than liquid particles.

  1. When a gas is cooled, the particles lose kinetic energy and move more slowly.
  2. As the gas particles slow down, they come closer together, and the attractive intermolecular forces between them become more significant.
  3. Once the particles are close enough, they begin to stick together, transitioning from a gas to a liquid. This process is called condensation.
An illustration showing the process of condensing, with a left panel labeled 'Gas' depicting scattered blue spheres and a right panel labeled 'Liquid' showing closely packed blue spheres. An arrow points from the gas to the liquid state.
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In a liquid, particles experience weaker electrostatic forces than in a solid, allowing them to move past each other, while remaining close together.

  1. When a liquid is cooled, the particles lose kinetic energy and move more slowly.
  2. As their kinetic energy decreases, the particles are less able to overcome the attractive intermolecular forces.
  3. Eventually, the particles become fixed in position, and the liquid freezes to form a solid.
An illustration showing the process of freezing. On the left, a cluster of blue circles labeled 'Liquid' represents particles in a liquid state, while on the right, a tightly packed arrangement of blue circles labeled 'Solid' represents particles in a solid state. An arrow points from the liquid to the solid state.
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Density is defined as mass per unit volume. According to the particle model, substances with particles that are further apart have a lower density. For most substances, the solid phase is denser than the liquid phase, which is denser than the gas phase.

Four squares showing particles in different arrangements, labeled from left to right: Low density, Medium density, Medium density, High density.

Water is unusual because its solid phase, ice, is less dense than liquid water.

When water freezes, its volume increases because the ice crystal structure forms with more open space between the water molecules than in the liquid state.

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The internal energy of a substance is the sum of the random distribution of kinetic and potential energies of its particles.

A table showing the movement, kinetic energy, and potential energy of solids, liquids, and gases. Under 'Movement', solids vibrate about fixed positions, liquids flow past each other, and gases move freely. The kinetic energy for solids is low, for liquids is medium, and for gases is high. The potential energy for solids is high, for liquids is medium, and for gases is low.

Particles in solids, liquids, and gases have potential energy due to the electrostatic attraction between the particles. This energy is negative because energy must be supplied to overcome the attractions.

Solids have the largest magnitude of negative potential energy, liquids have a lower magnitude, and gases have a negligible magnitude.

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When a substance is heated, its internal energy increases.

  • While a substance remains in the same phase, the heat energy supplied increases the average kinetic energy of its particles, causing the substance’s temperature to rise.
  • When the substance reaches its melting point or boiling point, the heat energy is used to weaken intermolecular bonds, increasing the particles’ potential energy and changing the phase of the substance, without changing the temperature.

This can be seen on a temperature–heat graph, which shows temperature rising between phase changes and remaining constant during melting or boiling.

A graph showing the relationship between Temperature and Heat. The graph includes labels for Melting point, Boiling point, Solid, Liquid, Gas, Freezing, Melting, Vaporizing, and Condensing.
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The transition of a substance from solid to liquid, and then to gas, involves changes in energy, bonding, and temperature:

1. Melting:

  • At the melting point, the supplied energy does not increase the temperature.
  • Instead, this energy is used to weaken the bonds within the solid structure.
  • This process makes the potential energies less negative, allowing the solid to melt into a liquid.

2. Heating the liquid:

  • Once melting is complete, continuous heating increases the liquid’s kinetic energy, causing its temperature to rise.

3. Vaporisation:

  • At the boiling point, the temperature remains constant.
  • The energy supplied weakens the intermolecular bonds.
  • The particle’s potential energies become less negative, and the liquid evaporates into a gas.

4. Heating the gas:

  • After all the liquid has vaporised, further heating increases the gas’s kinetic energy, resulting in a temperature rise.
A diagram illustrating the states of matter: Solid, Liquid, and Gas. Arrows indicate the processes of Melting, Freezing, Evaporating, and Condensing. The left side shows a densely packed arrangement of blue spheres representing Solid, the middle shows a more spaced arrangement for Liquid, and the right shows widely spaced spheres for Gas. The diagram also includes the phrases 'Add energy' and 'Remove energy'.

As a substance cools, internal energy decreases. Phase changes occur at the freezing or condensation points. Removing energy strengthens bonds, making potential energies more negative, reducing internal energy.

After the phase change, further cooling lowers the kinetic energy, resulting in a drop in temperature.

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As a substance is cooled, the average kinetic energy of its particles decreases. The temperature at which the average kinetic energy is zero is known as absolute zero, the lowest theoretical temperature.

The absolute (thermodynamic) scale starts at this point, so it has no negative values. The standard unit of temperature is the kelvin , one of the seven SI base units. The increment is the same as Celsius.

A thermometer showing three temperature levels: 373 K with steam, 273 K with ice, and 0 K labeled as absolute zero. Each temperature level is accompanied by a diagram of particles in motion.

On the absolute scale, temperature is directly proportional to the average kinetic energy of the particles in a substance. Therefore, doubling the absolute temperature doubles the average kinetic energy, regardless of the material. This is why the scale is independent of any particular substance.

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The equation relating the Kelvin and Celsius temperature scales can be used to find absolute zero () in degrees Celsius:

This also shows that the freezing point of pure water () in Kelvin is:

A more exact value for absolute zero is

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The internal energy of a substance is the sum of the random distribution of kinetic and potential energies of its particles (atoms or molecules).

As a substance is cooled, the average kinetic energy of the particles decreases. The temperature at which particles stop moving and have zero kinetic energy is called absolute zero (0 K), the lowest possible temperature.

However, at absolute zero, the particles still possess some potential energy due to electrostatic attractions between them, so the internal energy is never zero. Absolute zero is therefore the temperature at which a substance has the minimum internal energy due to the particles having zero kinetic energy and the smallest possible potential energy.

It is useful to know that the coldest natural temperature detected as of the time of writing is in the Boomerang Nebula (~1 K), while the lowest temperature achieved experimentally is around 1 picokelvin (1 pK) using ultracold atoms in laser and magnetic traps.

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