What make air a good insulator?

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    Air Insulator
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SUMMARY

Air is a good insulator primarily due to its low thermal conductivity and specific heat capacity, which is approximately 1.0084 kJ/kg·°C. Unlike materials that trap air and prevent convection, air's insulating properties stem from its kinetic energy transport, governed by the mean free path of gas molecules. The relationship between thermal conductivity, viscosity, and diffusivity is crucial in understanding heat transfer mechanisms in gases. Additionally, the specific heat capacity of air decreases with increasing molecular mass, influencing its overall insulating effectiveness.

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  • Understanding of thermal conductivity and its relation to heat transfer
  • Familiarity with the kinetic theory of gases
  • Knowledge of specific heat capacity and its calculation
  • Basic principles of convection in fluids
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Taylor_1989
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I am curious to know, what make air in itself a good insulator? Just to clarify I am not talking about materials that trap the air and stop the convection current from moving, from a hot surface to a cold one.

Is it because of the thermal capacity of air, which I believe is something like 1.0084 kg/c. My reason for thinking this is because air is classed as a fluid.

So when I look at something like an island surround by water it take the water long to lose it heat that the island due to have a higher heat capacity.
 
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Yup. Water has a very high heat capacity; air has a low capacity.
 
Thermal conductivity, like diffusivity, and viscosity is a transport phenomenon.

In the case of thermal conductivity, what is being transported is (average) kinetic energy, measured by the local temperature.

In the case of diffusivity, what is being transported is particles, measured by the local concentration.

In the case of viscosity, what is being transported is (average) momentum, measured by the flow velocity.

All these quantities are proportional, or, at least, correlated to one another for a given substance. In the kinetic theory of gases, a crucial quantity on which they depend is the mean free path. I will not give any derivation of these quantities, but merely point out some links:

Einstein equation for the diffusion coefficient. As you can see, it depends on the viscosity.

Similar correlations may be found between thermal conductivity and viscosity of gases. A search on Google reveals many papers published on this subject.

Molar specific heat capacity of a gas has a very simple form:

<br /> c_n \equiv \frac{C}{n} = \frac{f}{2} \, R<br />

But, if you want to find the specific heat capacity (per unit mass), you need to divide by the molar mass:
<br /> c_m \equiv \frac{C}{m} = \frac{C}{n} \, \frac{n}{m} = \frac{f}{2} \, \frac{R}{M}<br />
Thus, the more massive the molecules (atoms) of the gas, the smaller the specific heat capacity.

For mixtures, you need to take the averaged sum of the above expression.

One more thing, there is another mechanism for heat transfer in highly mobile fluids, and especially gases, namely, through convection. This means a macroscopic flux of a volume of a fluid between different points. As the volume of fluid moves, it carries its internal energy content, and exchanges it with its surrounding. In this mechanism, heat capacity may play a significant role.
 

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