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Observationally, the incremental increase of redshift with distance indicates that the wavelengths of light emitted from galaxies undergo a fractional increase. Therefore, for the ground state orbit of the Bohr atom, the wavelength K must increment in steps of some set fraction of K, say Kz R. This means that K z R. Furthermore, the wavelength increment D can be defined as Here, the term n is the new quantum integer that fulfils the same function as Bohrs quantum number n. Furthermore, Plancks quantum constant h finds its parallel in R. As a consequence, R could be called the Rydberg quantum wavelength since it is a specific fraction of the Rydberg wavelength. This designated fraction is given by the dimensionless number z which could perhaps be called the Rydberg quantum number. Analysis of the terms making up the Rydberg constant indicate Job vacancy closed job vacancy filled such a dimensionless number can indeed be obtained provided one reasonable assumption is made. The details are given in the main paper. This Rydberg quantum number z then bears the value Under these circumstances, the Rydberg quantum wavelength R is defined as This holds because of two factors. First, if n decreases with time, it will mimic the behaviour of the redshift, which also decreases with time. High redshift values from distant objects necessarily mean high values for n as well. Second, all atomic orbit radii r can be shown to remain unchanged throughout any quantum changes. If they were not, the abrupt change of size of every atom at the quantum jump would cause obvious flaws in crystals, which would be especially noticeable in ancient rocks. This new quantisation procedure effectively allows every atom in the cosmos to simultaneously Job vacancy closed job vacancy filled a new higher energy state for each of its orbits in proportion as the ZPE increases with time. In so doing, it opens the way for a solution to the redshift problem. In the Bohr atom, all orbit energies are scaled according to the energy of the orbit closest to the nucleus, the ground state orbit. Therefore, if the ground state orbit has an energy change, all other orbits will scale their energy proportionally. This also means that wavelengths of emitted light will be scaled in proportion to the energy of the ground state orbit of the atom. Accordingly, if W is the wavelength of the ground state orbit, then the wavelength change at the quantum jump is given by Now the redshift is defined as the change in wavelength, given by D, divided by the reference wavelength W. For the purposes of illustration, let us take the reference wavelength to be equal to that emitted when an electron falls into the ground state orbit for hydrogen. This wavelength is close to 1127 x 10 centimetres. For this orbit, the value of D from the above equation is given by 12072 x 10 This compares favourably with Tiffts basic value of 67 km/sec for the quantum jumps in the redshift velocity. Furthermore, when the new quantum number takes the value n 27, the redshift velocity Job vacancy closed job vacancy filled cz 72 km/sec compared with the 72 km/s that Tifft originally noticed. It may also be significant that for n 14, the redshift velocity is 39 Job vacancy closed job vacancy filled compared with Tiffts 2 km/s and 5 km/s that was subsequently established by Guthrie and Napier. Imposing a quantum condition on the second Bohr equation for the atom therefore produces quantum changes in orbit Job vacancy closed job vacancy filled and emitted wavelengths that accord with the observational evidence. This result also implies the quantised redshift may not be an indicator of universal expansion.