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Aktuelle Version vom 11. März 2026, 08:14 Uhr
An example of how we can go from diffraction to conical diffraction with diffracted rays using a green laser and the structure present in soap bubbles known as the Plateau border, tilting the angle of incidence of light φ (23°, 0°, and 20°). Using the angle θ of 4° to show the difference between the transmitted beam (LS) and the reflected beam (LD), therefore there is 8° between LS and LD. We can see that the diffraction cone also presents the reflection and refraction of light, which shows that we have the presence of the concept of diffracted rays. Light patterns are projections of parabolas from the conical scattering of light.
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| aktuell | 08:14, 11. Mär. 2026 |  | 1.310 × 1.071 (376 KB) | Nikolaos (Diskussion | Beiträge) | |
| 07:40, 11. Mär. 2026 |  | 640 × 525 (56 KB) | Nikolaos (Diskussion | Beiträge) | An example of how we can go from diffraction to conical diffraction with diffracted rays using a green laser and the structure present in soap bubbles known as the Plateau border, tilting the angle of incidence of light φ (23°, 0°, and 20°). Using the angle θ of 4° to show the difference between the transmitted beam (LS) and the reflected beam (LD), therefore there is 8° between LS and LD. We can see that the diffraction cone also presents the reflection and refraction of light, which shows tha… |
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