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Fig. 5. The prismatic spectrum observed at the different distances between the triangular prism and the screen: Castel [4], Wtinsch [56], Goethe [22], Werneburg [23], Cloquet [57], Nussbaumer [58].

Figure 5 The prismatic spectrum observed at the different distances between the triangular prism and the screen: Castel [4], Wtinsch [56], Goethe [22], Werneburg [23], Cloquet [57], Nussbaumer [58].

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Fig. 1. The hypothesis of the Descartes’ rotation energy of “globules” based on the knowledge of the 20" century: linear energy, rotation energy and geometric mean of both energies of colors. The data from Table I are graphically expressed in four ways as is shown in Fig. 1-4. Table I surveys the characteristic parameters of colors. Old Masters (Comenius and Lomonosow anticipated that the rotation speed of “globules” might be macroscopically measured as the temperature increase with the increasing rotation speed. Those measurements were done for different colors and led tc the discovery of the infrared radiation (e.g., Herschel in 1800). The data from Table I are graphically expressed in four wavs as is shown in Fig. 1-4.
Fig. 1. The hypothesis of the Descartes’ rotation energy of “globules” based on the knowledge of the 20" century: linear energy, rotation energy and geometric mean of both energies of colors. The data from Table I are graphically expressed in four ways as is shown in Fig. 1-4. Table I surveys the characteristic parameters of colors. Old Masters (Comenius and Lomonosow anticipated that the rotation speed of “globules” might be macroscopically measured as the temperature increase with the increasing rotation speed. Those measurements were done for different colors and led tc the discovery of the infrared radiation (e.g., Herschel in 1800). The data from Table I are graphically expressed in four wavs as is shown in Fig. 1-4.
Fig. 2. The hypothesis of the Descartes” rotation energy of “globules” based on the knowledge of the 20" century: “All color sensations can be referred to a common source; a simple rotating motion” (The prismatic spectrum is from Wikipedia)
Fig. 2. The hypothesis of the Descartes” rotation energy of “globules” based on the knowledge of the 20" century: “All color sensations can be referred to a common source; a simple rotating motion” (The prismatic spectrum is from Wikipedia)
Fig. 4. The hypothesis of the Descartes’ rotation energy of “globules” based on the knowledge of the 20" century: the growing rotation energy from ultraviolet color through visible colors to infrared color increases the macroscopic temperature of illuminated objects (The prismatic spectrum is from Wikipedia). Fig. 3. The hypothesis of the Descartes’ rotation energy of “globules” based on the knowledge of the 20th century: the growing rotation energy from ultraviolet color through visible colors to infrared color (many animals can see colors in the ultraviolet and infrared regions).
Fig. 4. The hypothesis of the Descartes’ rotation energy of “globules” based on the knowledge of the 20" century: the growing rotation energy from ultraviolet color through visible colors to infrared color increases the macroscopic temperature of illuminated objects (The prismatic spectrum is from Wikipedia). Fig. 3. The hypothesis of the Descartes’ rotation energy of “globules” based on the knowledge of the 20th century: the growing rotation energy from ultraviolet color through visible colors to infrared color (many animals can see colors in the ultraviolet and infrared regions).
Fig. 6. Goethe’s darkness (filled with ultraviolet and infrared photons) interacts with the white light behind the triangular prism get the Newtonian spectrum and the Goethean spectrum
Fig. 6. Goethe’s darkness (filled with ultraviolet and infrared photons) interacts with the white light behind the triangular prism get the Newtonian spectrum and the Goethean spectrum
Fig. 7. The lateral diffusion of the Descartes’ rotation energy of “globules”: the growing rotation energy from ultraviolet color through visible colors to infrared color modifies the white light with its initial rotation energy E,otation = 2.18 eV (Figure of prismatic colors from Wikipedia).
Fig. 7. The lateral diffusion of the Descartes’ rotation energy of “globules”: the growing rotation energy from ultraviolet color through visible colors to infrared color modifies the white light with its initial rotation energy E,otation = 2.18 eV (Figure of prismatic colors from Wikipedia).
This constructive color mixing of the red, green and blue colors is shown in Fig. 8. Fig. 8. The constructive mixing of red, green and blue colors with their constructive mixing angle 120° forms the white color.
This constructive color mixing of the red, green and blue colors is shown in Fig. 8. Fig. 8. The constructive mixing of red, green and blue colors with their constructive mixing angle 120° forms the white color.
Fig. 9. The destructive mixing of cyan, magenta and yellow colors with their destructive mixing angle 180° forms the black color. This destructive color mixing of the cyan, magenta and yellow colors is shown in Fig. 9.
Fig. 9. The destructive mixing of cyan, magenta and yellow colors with their destructive mixing angle 180° forms the black color. This destructive color mixing of the cyan, magenta and yellow colors is shown in Fig. 9.
Fig. 10. The compound magenta color is decomposed in the darkroom to its components. The compound magenta color in the light cabinet transfers the rotation energy of their components to neutral white photons with a single wavelength. This preparation of magenta leads to its immutability.
Fig. 10. The compound magenta color is decomposed in the darkroom to its components. The compound magenta color in the light cabinet transfers the rotation energy of their components to neutral white photons with a single wavelength. This preparation of magenta leads to its immutability.
Fig. 11. The compound cyan color is decomposed in the darkroom to its components. The compound cyan color in the light cabinet transfers the rotation energy of their components to neutral white photons with a single wavelength. This preparation of cyan leads to its immutability.
Fig. 11. The compound cyan color is decomposed in the darkroom to its components. The compound cyan color in the light cabinet transfers the rotation energy of their components to neutral white photons with a single wavelength. This preparation of cyan leads to its immutability.
Fig. 12. The compound yellow color is decomposed in the darkroom to its components. The compound yellow color in the light cabinet transfers the rotation energy of their components to neutral white photons with a single wavelength. This preparation of yellow leads to its immutability.
Fig. 12. The compound yellow color is decomposed in the darkroom to its components. The compound yellow color in the light cabinet transfers the rotation energy of their components to neutral white photons with a single wavelength. This preparation of yellow leads to its immutability.
Fig. 13. Reflectance spectra of different combinations of wavelengths leading to the “correct” yellow color. The average value of all rotation energies of present photons determines the final color. Inspired by Pehr Sallstrém [64]. In some cases, the resulting observed color can be determined from a wide range of wavelengths and it is possible to “create” a color even without the “right” wavelengths. E.g., it is possible to “prepare” the yellow color without the wavelengths within the range 570-590 nm. Fig. 13 documents situations with various wavelengths compositions leading to a “correct” yellow color. In order to solve this dilemma, we propose that the value of the average rotation energy of all visible photons decides the final color.
Fig. 13. Reflectance spectra of different combinations of wavelengths leading to the “correct” yellow color. The average value of all rotation energies of present photons determines the final color. Inspired by Pehr Sallstrém [64]. In some cases, the resulting observed color can be determined from a wide range of wavelengths and it is possible to “create” a color even without the “right” wavelengths. E.g., it is possible to “prepare” the yellow color without the wavelengths within the range 570-590 nm. Fig. 13 documents situations with various wavelengths compositions leading to a “correct” yellow color. In order to solve this dilemma, we propose that the value of the average rotation energy of all visible photons decides the final color.
Fig. 14. Six new prismatic spectra discovered by Nussbaumer in 2008 [28]. EEA SAS ESR LORE Eg aS Se ARESENS SRS Te | “EN Based on the Descartes’ rotation energy of visible photons we predict that the observed white color appears as the constructive interference of colors. On the other side, the observed black color might be the result of the destructive interference of colors. The composition of spectra varied with the distance from the observed original color combination. The detailed experimental and theoretical investigation of these impressive spectra have to be done in the future. IX. CONCLUSION
Fig. 14. Six new prismatic spectra discovered by Nussbaumer in 2008 [28]. EEA SAS ESR LORE Eg aS Se ARESENS SRS Te | “EN Based on the Descartes’ rotation energy of visible photons we predict that the observed white color appears as the constructive interference of colors. On the other side, the observed black color might be the result of the destructive interference of colors. The composition of spectra varied with the distance from the observed original color combination. The detailed experimental and theoretical investigation of these impressive spectra have to be done in the future. IX. CONCLUSION
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