add notes on thermal expansion, thermal conductivity
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@ -631,3 +631,143 @@ bonds between the surface of the fibre and matrix.
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Kevlar/Epoxy | 1200 | 20
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(All units in MPa)
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# Thermal Properties of Materials
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## Specific Heat Capacity
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How much heat energy is required to raise the temperature of a body by one unit:
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$$ C_p = \frac{\Delta E}{m\Delta T} $$
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where $c$ is specific heat capacity.
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It is measured at a constant pressure, usually $1.013\times 10^5$ Pa.
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## Molar Heat Capacity
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$$C_pm = \frac{\Delta E}{n\Delta T}$$
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<details>
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<summary>
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#### What is a mole?
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</summary>
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> The mole (symbol: mol) is the base unit of amount of substance in the International System of
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> Units (SI).
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> It is defined as exactly $6.02214076\times 10^{23}$ elementary entities ("particles")
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~ [Wikipedia: Mole (unit)](https://en.wikipedia.org/wiki/Mole_(unit))
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<details>
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<details>
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<summary>
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#### How Much Does a mol of Something weigh?
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</summary>
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A mol of an element weighs its relative atomic mass ($A_r$) but in grams.
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For example, Carbon-12 has an $A_r$ of 12 (as it's made of 6 neutrons, 6 protons, and 6 electrons
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which have negligible mass) so a mol of Carbon-12 has a mass of 12 g.
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</details>
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## Thermal Expansion
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<details>
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<summary>
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### Origin of Thermal Expansion
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</summary>
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All atomic bonds vibrate, on the magnitude of gigahertz.
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The bonds vibrate about a mean positoin and the vibration is a simple harmonic motion.
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From the graph below you can see that as energy (in the form of heat) is supplied to the bonds,
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the amplitude of the vibrations get larger and larger.
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You can also see the mean position of the bond gets further and further away, meaning the volume
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of the material also is increasing.
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The mean position of the bond is what dictates the volume, as this means the inter-atomic
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separation increases.
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![Morse Potential Graph](./images/vimscrot-2021-12-21T19:51:58,667328620+00:00.png)
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Morse potential is the energy well between 2 bonded atoms.
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The graph is asymmetric due to the repulsion experienced by atoms as they apporach.
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</details>
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### Linear Coefficient of Thermal Expansion
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$$\alpha_L = \frac{\Delta L}{L_0 \Delta T}$$
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where $L$ is the sample length.
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<details>
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<summary>
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#### Example 1
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A 1 m long bar of aluminium metal cools in the solid state from 660 \textdegree{}C to
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25 \textdegree{}C.
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Calculate the length of the bar after it cools down, given $\alpha_L = 25\times10^{-6}$ K$^{-1}$.
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</summary>
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\begin{align*}
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l_0 &= 1 \\
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\Delta T &= T_f - T_0 = 25 - 660 = -635 \\
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\\
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\alpha_L &= \frac{l_f - l_0}{l_0 \Delta T} \\
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\alpha_L l_0 \Delta T &= l_f - l_0 \\
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l_f &= \alpha_L l_0 \Delta T + l_0 = 0.984
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\end{align*}
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</details>
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### Linear Thermal Expansion and Isotropism
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Since isotropic solids have the same properties in all directions, you can say that for an
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isotropic solid:
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$$\alpha_V = 3\alpha_L = \frac{\Delta V}{V_0 \Delta T}$$
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### Reasons to Care About Thermal Expansion
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- A coating on a material may fail if the thermal expansion coefficients do not match
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- A brittle material may thermally shock and fracture due to thermal expansion mismatch between
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the ouside and inside, especially if the material is not very thermally conductive
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## Thermal Conductivity
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Thermal conductivity is the rate at which heat power is transferred through a material.
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$$\frac{Q}{A} = k \frac{\Delta T}{\Delta x}$$
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where $Q$ is heat power, $A$ is area of the surface, $\frac{\Delta T}{\Delta x}$ is the
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temperature gradient, and $k$ is the thermal conductivity constant.
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<details>
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<summary>
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### Origin of Thermal Conductivity
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</summary>
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Heat is transferred through materials by electrons (and partially by atomic vibrations)
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Metals have high thermal conductivity as their delocalised 'sea' electrons are about to move about
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easily.
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This makes them excellent conductors of heat and electricity.
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Ceramics, glasses, and polymers do not have delocalised electrons and are therefore poor conductors
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of heat and electricity (they are insulators).
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Polymer foams are even better insulators because they have holes which lowers their density.
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</details>
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