Is it possible to develop a entirely new method of measuring temperature that starts at absolute zero, and isn't really built around the freezing point or boiling point of something, but instead is based purely on average kinetic (heat) levels?
We already have it. The absolute temperature (kelvins, K) . The amplitude of a kelvin is the same as that of 1º C.
There are many definitions of temperature. The most general one, which arises from statistical physics, is
[latex]
\[
T=\left(\frac{\partial U}{\partial S}\right)_V
\]
[/latex]
But basic thermodynamics can give us an
operational definition, useful to define practical
thermometric scales. We first go to the Law 0 of Thermodynamics, about thermal equilibrium[1]. We give a number to all the states of a system in thermal equilibrium (isotherm). In general, this allows us to define a function of physical parameters that is constant for states in thermal equilibrium. For example, for an ideal gas, all the states with
[latex]
\[
P_1V_1=P_2V_2=P_3V_3=\ldots
\]
[/latex]
define an isotherm. So we can say that a and b are in thermal equilibrium if
P_aV_a = P_b V_b. The next step is to say theta = PV, we label each isotherm with some number. This number is going to be the empirical temperature.
For an ideal gas, the thermometric property is PV, other systems have different thermometric properties
- Column of mercury, alcohol ... in a glass tube -> length.
- Pyrometer -> Stefan-Boltzmann law
- Resistance thermometer.
- Quarz crystal -> vibration frecuency
- Magnetic thermometer -> magnetic susceptibility
- Thermoelectric pair -> emf
- ...
Any of these can provide an empirical definition of temperature. We can say that temperature is the length of the liquid column or the vibration frequency. In general we choose a function, usually linear, [latex]\footnotesize $\theta=ax+b$[/latex] of the thermometric property. To fix the scale we choose two arbitray points and give them values (boiling and freezing point of water, for example). Another alternative is to set b = 0 and choose only a single point. This is what we do nowadays. We measure temperature in kelvins and define a kelvin as 1/273.16 of the temperature of the triple point of water (a state that only happens at a particular pressure where water, vapour and ice are in equilibirum, it's just over 0º C).
Now we have theta = 273.16 x / x_3, where x is some thermometric property and x_3 its value at the triple point. For example, imagine a thermoelectric pair that indicates 2.17 mV at the triple point. If for a certain system we get 6.02 mV, we know the temperature is 273.16*6.02/2.17 = 757.8 K.
The best thermometer we have is the constant volume gas thermometer. The thermometric property is pressure, and the temperature is
[latex]
\[
\theta = T = 273.16 \lim_{p_3\to0}\frac{p}{p_3}
\]
[/latex]
Where T is the ideal gas absolute temperature.
In practice, we cannot use this system all the time, although it is the primary thermometer. The standard scale is called ITS-90 and it is based in many reproducible fixed points, of which only the triple point of water is exact by definition. The thermometer changes for different temperature ranges. Some fixed points are
[latex]
\sffamily\footnotesize
\begin{tabular}{lcc}
\hline
\bfseries Fixed point & $T$ (K) & t ($^\circ$ C)\\
\hline
Helium vapour pressure & 3--5 & -270.15---268.16\\
Hydrogen triple point & 13.80 & -259.35\\
Neon triple point & 24.56 & -248.59\\
Oxygen triple point & 54.36 & -218.79\\
\ldots\\
Water triple point & 273.16 & 0.01\\
\ldots\\
Zinc melting point & 692.67 & 419.53\\
\ldots\\
Gold melting point & 1337.33 & 1064.18\\
\ldots
\end{tabular}
[/latex]
The helium gas thermometer is used until the triple point of neon. Then comes the platinum resistence thermometer, until the melting point of silver and finally radiation thermometers are used.
In short, the theoretical general definition of temperature, and the one a theoretical physicist uses, is
[latex]
\[
T=\left(\frac{\partial U}{\partial S}\right)_V
\]
[/latex]
Which matches your ideas. But a practical definition of a scale that allows for precise measurements over a large range is more involved and requires several stages.
_____
[1] Thermal equilibrium means that the thermodynamical variables of the system remain constant.