We can extend the one-dimensional model of an electron to make an example of a two-dimensional space. Just sort the electron's quarks into four clumps as shown in the accompanying diagram and determine the electric polarity $\delta _{\hat{e}}$ of each clump from the coefficients of electronic quarks. Remember that vectors that are scalar multiples of $\hat{e} \equiv (0, 1, 0)$ are collectively called the electric axis, and objectify any difference in $\delta _{\hat{e}}$ as a variation in direction on this electric axis. Characterize a range of locations using the orbital radius $R$. Then combine the electric axis with the polar axis to make a *two*-dimensional model. This construction is called two-dimensional because the description is objectified from two classes of sensation which may vary independently from each other.

A look around a two-dimensional quark model of the electron. |

To illustrate, we add another rod to represent the electric axis as shown in the accompanying movie. The polar and electric axes are displayed perpendicular to each other as a visual representation of their logical independence. The model is two-dimensional because it displays variations in background brightness along the polar axis, and differences in yellowness along the electric axis. Quarks are shown in different quadrants as a visual depiction of how Pauli's exclusion principle is satisfied for baryonic and rotating quarks. Different locations are used to portray differences in the electric polarity $\delta _{\hat{e}}$ and the phase $\delta _{\theta}$.