$$E=\frac{l^2m}{t^2}$$
where \(l\) is length (already defined in \(Å\)), \(m\) is mass (already defined in \(Da\)), and \(t\) is time.
Notice how we still need to define which unit is going to be used to measure time. It is customary
to use the picosecond (\(ps\)) in MD because it produces results with magnitudes within \(1×10^{-4} < x_i < 1×10^4\) when used in combination with the \(Å\) and the \(Da\).
If we want to calculate the kinetic temperature of the system using the following relation:
$$T_{kinetic}=\frac{2\bar{K_E}}{3k_b}$$
where \(\bar{K_E}\) is the kinetic energy of the particles and \(k_b\) is the Boltzmann constant,
we would have to define the unit to measure temperature (\(T\)) as well. We can use the Kelvin (\(K\)) and make sure to convert \(k_b\) to the system of units that we have defined until now.
\(k_b\) would be equal to \(0.831036 Å^2Da/{ps^2K}\).
In conclusion, our custom system of fundamental units selected for this example is defined by:
the angstrom \(Å\) to measure length, the Dalton \(Da\) to measure mass, the picosecond \(ps\) to measure time, and Kelvin \(K\) to
measure temperature. Any quantity inputted into Scymol would have to be converted to this system of units. In return, any
quantity returned by Scymol will be based on this unit system. For example, the velocities of the particles would be measured in \(Å/{ps}\), acceleration in \(Å/{ps^2}\), force in \(mÅ/{ps^2}\), energy in \(mÅ^2/{ps^2}\),
and temperature in \(K\). A conversion list from this system of units to SI is found in Table 2 (page 1).
Post-processing tools included in Scymol would output quantities that rely on these custom units as well, as seen in Figure 1.