**Thermal expansion** is a physical property of a substance (gas, liquid or solid) to modify its shape (length, area or volume) function of temperature. Thermal expansion relates with the expansion and contraction of particles in a substance function of temperature.

Thermal expansion can also be regarded as a fractional change in size of a material/substance caused by a change of temperature.

Thermal expansion has effect on gases, liquids and solids. From the mathematical point of view, thermal expansion can be described as:

**linear**(one direction, 1-D)**areal**(two directions, 2-D)**volumetric**(three directions, 3-D)

The linear and areal (also called superficial) thermal expansion applies only to solids. The volumetric (also called cubical) thermal expansion applies to both solids and liquids. For gases, thermal expansion is described by the **ideal gas law** and it is treated differently.

### Linear thermal expansion

Linear thermal expansion applies mostly to solids. Knowing the **initial length** L_{0} [m] of a given solid (e.g. metal rod), the **temperature difference** ΔT [ºC] and the **coefficient of linear expansion** of the solid α [1/ºC], the change in length ΔT [m] of the solid can be calculated as:

The change in length is directly proportional with the change in temperature. The higher the temperature difference the higher the increase in length of the material (e.g. metal rod).

The **length difference** ΔL is equal with the subtraction of the initial length L_{0} from the final length L:

By replacing (2) in (1), we can calculate the **final length** (after thermal expansion) function of the initial length, temperature difference and linear thermal expansion coefficient.

The coefficient of linear thermal expansion is not constant but varies slightly with temperature. Therefore, the mathematical expression can be applied only to small temperature variations.

### Areal thermal expansion

Thermal expansion also applies to surfaces. Imagine a sheet of metal with a defined area. If heated, the same sheet of metal will have a slightly bigger area.

Knowing the **initial area** A_{0} [m^{2}] of a given solid (e.g. metal sheet), the **temperature difference** ΔT [ºC] and the **coefficient of linear expansion** of the solid α [1/ºC], the change in area ΔA [m^{2}] of the solid can be calculated as:

The change in area is directly proportional with the change in temperature. The higher the temperature difference the higher the increase in surface of the material (e.g. metal sheet).

The **area difference** ΔA is equal with the subtraction of the initial area A_{0} from the **final area** A:

By replacing (5) in (4), we can calculate the final area (after thermal expansion) function of the initial area, temperature difference and linear thermal expansion coefficient.

\[\bbox[#FFFF9D]{A = A_0 \cdot (1+ 2 \cdot \alpha \cdot \Delta T)} \tag{6}\]To demonstrate the mathematical expression (6), let’s assume that the area is the square of the length:

\[A = L^2 \tag{7}\]Replacing (3) in (7), gives:

\[A = L_{0}^2 \cdot \left ( 1 + 2 \cdot \alpha \cdot \Delta T + \alpha^2 \cdot \Delta T^2 \right ) \tag{8}\]Since the coefficient of thermal expansion is very small (e.g. for steel 12·10^{-6} 1/ºC), the quadratic term of the equation (8) can be neglected. Assuming that the initial area is equal with the square of the initial length:

equation (8) becomes (6).

The same principle applies to areal thermal expansions. The coefficient of linear thermal expansion is not constant but varies slightly with temperature. Therefore, the mathematical expression can be applied only to small temperature variations.

### Volumetric thermal expansion

Thermal expansion causes variations in volume for solids and liquids function of temperature.

Knowing the **initial volume** V_{0} [m^{3}] of a given solid, the **temperature difference** ΔT [ºC] and the **coefficient of linear expansion** of the solid α [1/ºC], the change in volume ΔV [m^{3}] of the solid can be calculated as:

The change in volume is directly proportional with the change in temperature. The higher the temperature difference the higher the increase in volume of the material.

The **volume difference** ΔV is equal with the subtraction of the initial volume V_{0} from the **final volume** V:

By replacing (11) in (10), we can calculate the final volume (after thermal expansion) function of the initial volume, temperature difference and linear thermal expansion coefficient.

\[\bbox[#FFFF9D]{V = V_0 \cdot (1+ 3 \cdot \alpha \cdot \Delta T)} \tag{12}\]To demonstrate the mathematical expression (12), let’s assume that the volume is the cube of the length:

\[V = L^3 \tag{12}\]Replacing (3) in (12), gives:

\[V = L_{0}^3 \cdot \left ( 1 + 3 \cdot \alpha \cdot \Delta T + 3 \cdot \alpha^2 \cdot \Delta T^2 + \alpha^3 \cdot \Delta T^3 \right ) \tag{14}\]Since the coefficient of thermal expansion is very small, the cubic and quadratic terms of the equation (14) can be neglected. Assuming that the initial volume is equal with the cube of the initial lenght:

\[V_0 = L_{0}^3 \tag{15}\]equation (14) becomes (12).

For volumetric thermal expansion calculations we can use the **coefficient of volumetric thermal expansion** β instead of the **coefficient of linear thermal expansion** α.

which gives the equation for the change in volume:

\[\bbox[#FFFF9D]{\Delta V = \beta \cdot V_0 \cdot \Delta T} \tag{17}\]The same principle applies to volumetric thermal expansions. The coefficient of volumetric thermal expansion is not constant but varies slightly with temperature. Therefore, the mathematical expression can be applied only to small temperature variations.

The coefficient of thermal expansion are obtained from **experimental data**. In the table below you can find the values of the thermal expansion coefficient for common substances.

Material | Coefficient of linear expansion | Coefficient of volume expansion |

Solids | ||

Aluminum | 25·10^{-6} | 75·10^{-6} |

Brass | 19·10^{-6} | 56·10^{-6} |

Copper | 17·10^{-6} | 51·10^{-6} |

Gold | 14·10^{-6} | 42·10^{-6} |

Iron | 12·10^{-6} | 35·10^{-6} |

Invar | 0.9·10^{-6} | 2.7·10^{-6} |

Lead | 29·10^{-6} | 87·10^{-6} |

Silver | 18·10^{-6} | 54·10^{-6} |

Glass | 9·10^{-6} | 27·10^{-6} |

Glass | 3·10^{-6} | 9·10^{-6} |

Quartz | 0.4·10^{-6} | 1·10^{-6} |

Concrete | 12·10^{-6} | 36·10^{-6} |

Marble | 7·10^{-6} | 21·10^{-6} |

Liquids | ||

Ether | 1650·10^{-6} | |

Ethyl | 1100·10^{-6} | |

Petrol | 950·10^{-6} | |

Glycerin | 500·10^{-6} | |

Mercury | 180·10^{-6} | |

Water | 210·10^{-6} | |

Gases | ||

Air and most other gases at atmospheric pressure | 3400·10^{-6} |

Source:

College Physics, openstax, Rice University

Wikipedia

### Thermal expansion examples

**Example 1 (linear thermal expansion)**. Assuming a bridge, made of steel, with an initial total length of 1500 m at -20 ºC, calculate the length difference at 40 ºC and its total length.

**Step 1**. Write down the known parameters of the problem:

L_0 &= 1500 \text{ m}\\

T_0 &= -20 \text{ }^\circ \text{C}\\

T &= 40 \text{ }^\circ \text{C}\\

\alpha &= 12 \cdot 10^{-6} \text{ 1/}^\circ \text{C}

\end{split} \]

**Step 2**. Calculate the temperature difference

**Step 3**. Calculate the length difference

**Step 4**. Calculate the total final length

The change in length is very small compared with the initial length of the bridge. However it’s noticeable and can cause structural problems if not taken into account in the **design phase**. Because of the thermal expansion, metal bridges are build up from several sections which have air gaps between them, in order to allow thermal expansion function of temperature change.

Thermal expansion has also a big impact on railway tracks. A 10 km railway track is not made up from a single piece of steel but divided into several pieces with air gaps (expansion spaces) between them. In winter the air gaps are bigger becasue the rails have smaller length and in summer the air gaps are bearly noticeable becasue the rails have increase length due to thermal expansion.

**Example 2 (area thermal expansion)**. Assuming a football pitch is made of aluminium and has an initial total area of 7140 m^{2} at -10 ºC, calculate the area difference at 30 ºC and its total area.

**Step 1**. Write down the known parameters of the problem:

A_0 &= 7140 \text{ m}^2\\

T_0 &= -10 \text{ }^\circ \text{C}\\

T &= 30 \text{ }^\circ \text{C}\\

\alpha &= 25 \cdot 10^{-6} \text{ 1/}^\circ \text{C}

\end{split} \]

**Step 2**. Calculate the temperature difference

**Step 3**. Calculate the area difference

**Step 4**. Calculate the total final area

**Example 3 (volumetric thermal expansion)**. For this example we are going to assume that we have a 50 L steel tank full with gasoline at -20 ºC. What is going to be the volume difference for both tank and fuel at 40 ºC? Is the fuel going to fit in the fuel tank?

**Step 1**. Write down the known parameters of the problem:

V_{0t} &= 50 \text{ L}\\

V_{0f} &= 50 \text{ L}\\

T_0 &= -20 \text{ }^\circ \text{C}\\

T &= 40 \text{ }^\circ \text{C}\\

\alpha &= 12 \cdot 10^{-6} \text{ 1/}^\circ \text{C}\\

\beta &= 950 \cdot 10^{-6} \text{ 1/}^\circ \text{C}\\

\end{split} \]

**Step 2**. Calculate the temperature difference

**Step 3**. Calculate the volume difference of the fuel tank (assuming it’s solid steel)

**Step 4**. Calculate the volume difference of the fuel (gasoline)

**Step 5**. Calculate the excess volume of fuel

We can see that there is more fuel than the full capacity of the tank, which means that the excess fuel will spill.

You can also check your results using the calculator below.

### Thermal Expansion Calculator

L_{0} [m] | α [1/°C] | T_{0} [°C] | T [°C] | Linear expasion | L [m] = | |

ΔL [m] = | ||||||

A_{0} [m^{2}] | α [1/°C] | T_{0} [°C] | T [°C] | Areal expasion | A [m^{2}] = | |

ΔA [m^{2}] = | ||||||

V_{0} [m^{3}] | α [1/°C] | T_{0} [°C] | T [°C] | Volumetric solid expasion | V [m^{3}] = | |

ΔV [m^{3}] = | ||||||

V_{0} [m^{3}] | β [1/°C] | T_{0} [°C] | T [°C] | Volumetric gas expasion | V [m^{3}] = | |

ΔV [m^{3}] = |

### Bimetallic Strips

A bimetallic strip is made up from two metals, bond together, with different thermal expansion coefficient.

The two strips of metal are bond together at a reference temperature (e.g. 20 °C), having equal lengths. When the temperature change, because they have different thermal expansion coefficient, the length change (ΔL) of each strip will be different. Being bond together, the strip will bend function of temperature change.

Bimetallic are used as switches in electric circuits to open/close electric contacts function of external temperature or current through the circuit.

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## Kelvin Saw

Appreciate if you could help to calculate. If the pillar height is 4.473 meter. What should the best maximum height limits we should set with the consideration of thermal expansion? It is 4.2 meter is good to use?

## ain

hi, correct me if i am wrong….suppose example 2….the solution to find delta A…should multiply with 2 alpha????