Test One Solutions To Course Four, Part 1

1) The Heisenburg Exclusion Principle holds true foremost because electrons are constantly bombarded by incoming electromagnetic energy that tends to associate with the described electrons in a random manner. Electrons are a relatively point mass that exists as particle, wave, and energy all at the same time. So, even if you were to have selective electromagnetic energy to interact with an electron, once you were to identify the given electron as a particle, the electron's wave and energy qualities would alter your ability to detect the given electron. This is particularly since an electron always needs to move at close to light speed in order to be an electron.

2) Any sort of identification of an electron at a locus of region would indicate that the spin, orbit, and angular momentum of that electron as it moves transversely forms a surface area of the given electron that relatively tends to orthogonally "throw" off phenomena that attempts to interact with the said electron in a directoralization that is existent in a given manner when one includes the overall Fourier Translation of the given electron through its kinematically based Lagrangian in space and time.

3) A sports related ball that spins, orbits, and moves transversely in a circular path will tend to throw off the air that interacts with the said ball in a multiplicitly orthogonal manner when considering the overall translation of that ball in time and space. The prior would only exist with an integer number of sports related balls. So, you couldn't have 1 and 1/2 balls doing this, since the balls here are considered discrete phenomena.

4) The angular momentum of an electron forms its electric field, while the spin-orbital momentum of an electron forms its magnetic field. J = L cross S. This means that the momentum of an electron equals its angular momentum cross its spin-orbital momentum.

5) The momentum of electrons (J) is formed in part by the attraction of the electrons with protons. As the electrons have a momentum given to them that is a drive in a direction (angular momentum) that also spins in two relative orthogonal manners so as to counter intruding forces (magnetic field produced by spin-orbital momentum), the holomorphic directoralization of this overall momentum pulls the electrons around the nuclei in a circular propagation.