add notes on thermal expansion, thermal conductivity
This commit is contained in:
parent
c7122f797d
commit
60f81709c2
Binary file not shown.
After Width: | Height: | Size: 128 KiB |
@ -631,3 +631,143 @@ bonds between the surface of the fibre and matrix.
|
|||||||
Kevlar/Epoxy | 1200 | 20
|
Kevlar/Epoxy | 1200 | 20
|
||||||
|
|
||||||
(All units in MPa)
|
(All units in MPa)
|
||||||
|
|
||||||
|
# Thermal Properties of Materials
|
||||||
|
|
||||||
|
## Specific Heat Capacity
|
||||||
|
|
||||||
|
How much heat energy is required to raise the temperature of a body by one unit:
|
||||||
|
|
||||||
|
$$ C_p = \frac{\Delta E}{m\Delta T} $$
|
||||||
|
|
||||||
|
where $c$ is specific heat capacity.
|
||||||
|
|
||||||
|
It is measured at a constant pressure, usually $1.013\times 10^5$ Pa.
|
||||||
|
|
||||||
|
## Molar Heat Capacity
|
||||||
|
|
||||||
|
$$C_pm = \frac{\Delta E}{n\Delta T}$$
|
||||||
|
|
||||||
|
<details>
|
||||||
|
<summary>
|
||||||
|
|
||||||
|
#### What is a mole?
|
||||||
|
|
||||||
|
</summary>
|
||||||
|
|
||||||
|
> The mole (symbol: mol) is the base unit of amount of substance in the International System of
|
||||||
|
> Units (SI).
|
||||||
|
> It is defined as exactly $6.02214076\times 10^{23}$ elementary entities ("particles")
|
||||||
|
|
||||||
|
~ [Wikipedia: Mole (unit)](https://en.wikipedia.org/wiki/Mole_(unit))
|
||||||
|
|
||||||
|
<details>
|
||||||
|
|
||||||
|
<details>
|
||||||
|
<summary>
|
||||||
|
|
||||||
|
#### How Much Does a mol of Something weigh?
|
||||||
|
|
||||||
|
</summary>
|
||||||
|
|
||||||
|
A mol of an element weighs its relative atomic mass ($A_r$) but in grams.
|
||||||
|
For example, Carbon-12 has an $A_r$ of 12 (as it's made of 6 neutrons, 6 protons, and 6 electrons
|
||||||
|
which have negligible mass) so a mol of Carbon-12 has a mass of 12 g.
|
||||||
|
|
||||||
|
</details>
|
||||||
|
|
||||||
|
## Thermal Expansion
|
||||||
|
|
||||||
|
<details>
|
||||||
|
<summary>
|
||||||
|
|
||||||
|
### Origin of Thermal Expansion
|
||||||
|
|
||||||
|
</summary>
|
||||||
|
|
||||||
|
All atomic bonds vibrate, on the magnitude of gigahertz.
|
||||||
|
The bonds vibrate about a mean positoin and the vibration is a simple harmonic motion.
|
||||||
|
|
||||||
|
From the graph below you can see that as energy (in the form of heat) is supplied to the bonds,
|
||||||
|
the amplitude of the vibrations get larger and larger.
|
||||||
|
You can also see the mean position of the bond gets further and further away, meaning the volume
|
||||||
|
of the material also is increasing.
|
||||||
|
The mean position of the bond is what dictates the volume, as this means the inter-atomic
|
||||||
|
separation increases.
|
||||||
|
|
||||||
|
![Morse Potential Graph](./images/vimscrot-2021-12-21T19:51:58,667328620+00:00.png)
|
||||||
|
|
||||||
|
Morse potential is the energy well between 2 bonded atoms.
|
||||||
|
The graph is asymmetric due to the repulsion experienced by atoms as they apporach.
|
||||||
|
|
||||||
|
</details>
|
||||||
|
|
||||||
|
### Linear Coefficient of Thermal Expansion
|
||||||
|
|
||||||
|
$$\alpha_L = \frac{\Delta L}{L_0 \Delta T}$$
|
||||||
|
|
||||||
|
where $L$ is the sample length.
|
||||||
|
|
||||||
|
<details>
|
||||||
|
<summary>
|
||||||
|
|
||||||
|
#### Example 1
|
||||||
|
|
||||||
|
A 1 m long bar of aluminium metal cools in the solid state from 660 \textdegree{}C to
|
||||||
|
25 \textdegree{}C.
|
||||||
|
Calculate the length of the bar after it cools down, given $\alpha_L = 25\times10^{-6}$ K$^{-1}$.
|
||||||
|
|
||||||
|
</summary>
|
||||||
|
|
||||||
|
\begin{align*}
|
||||||
|
l_0 &= 1 \\
|
||||||
|
\Delta T &= T_f - T_0 = 25 - 660 = -635 \\
|
||||||
|
\\
|
||||||
|
\alpha_L &= \frac{l_f - l_0}{l_0 \Delta T} \\
|
||||||
|
\alpha_L l_0 \Delta T &= l_f - l_0 \\
|
||||||
|
l_f &= \alpha_L l_0 \Delta T + l_0 = 0.984
|
||||||
|
\end{align*}
|
||||||
|
|
||||||
|
</details>
|
||||||
|
|
||||||
|
### Linear Thermal Expansion and Isotropism
|
||||||
|
|
||||||
|
Since isotropic solids have the same properties in all directions, you can say that for an
|
||||||
|
isotropic solid:
|
||||||
|
|
||||||
|
$$\alpha_V = 3\alpha_L = \frac{\Delta V}{V_0 \Delta T}$$
|
||||||
|
|
||||||
|
### Reasons to Care About Thermal Expansion
|
||||||
|
|
||||||
|
- A coating on a material may fail if the thermal expansion coefficients do not match
|
||||||
|
- A brittle material may thermally shock and fracture due to thermal expansion mismatch between
|
||||||
|
the ouside and inside, especially if the material is not very thermally conductive
|
||||||
|
|
||||||
|
## Thermal Conductivity
|
||||||
|
|
||||||
|
Thermal conductivity is the rate at which heat power is transferred through a material.
|
||||||
|
|
||||||
|
$$\frac{Q}{A} = k \frac{\Delta T}{\Delta x}$$
|
||||||
|
|
||||||
|
where $Q$ is heat power, $A$ is area of the surface, $\frac{\Delta T}{\Delta x}$ is the
|
||||||
|
temperature gradient, and $k$ is the thermal conductivity constant.
|
||||||
|
|
||||||
|
<details>
|
||||||
|
<summary>
|
||||||
|
|
||||||
|
### Origin of Thermal Conductivity
|
||||||
|
|
||||||
|
</summary>
|
||||||
|
|
||||||
|
Heat is transferred through materials by electrons (and partially by atomic vibrations)
|
||||||
|
|
||||||
|
Metals have high thermal conductivity as their delocalised 'sea' electrons are about to move about
|
||||||
|
easily.
|
||||||
|
This makes them excellent conductors of heat and electricity.
|
||||||
|
|
||||||
|
Ceramics, glasses, and polymers do not have delocalised electrons and are therefore poor conductors
|
||||||
|
of heat and electricity (they are insulators).
|
||||||
|
|
||||||
|
Polymer foams are even better insulators because they have holes which lowers their density.
|
||||||
|
|
||||||
|
</details>
|
||||||
|
Loading…
Reference in New Issue
Block a user