Young’s double-slit interference experiment is a classic optical experiment in the College Optical-Physics Experiments. In 1801, Thomas Young (1773-1829) conducted an interference experiment of light, known as Young's two-hole interference experiment, and confirmed the wave character of light for the first time. Later, he established a new wave theory based on the interference principle, explained Newton’ in his papers s ring, and accurately measured the wavelength in his papers. In Young’s double-slit experiment, since there is a small slit s, light waves arriving at s become two secondary wave sources that transmits cylindrical waves. And they transmit one secondary cylindrical wave, respectively. The two secondary waves have the same frequency, since they come from the same wave surface. The vibration directions of s1 and s2 are approximate due to the close distance between them. Since the vibration phase differences of s1 and s2 remain constant, the two light waves meet the coherent condition, thus forming interference fringes on the screen. This is a typical optical experiment that obtains coherent optical waves using the wavefront splitting method.
Through building the Young’s double-slit interference cage system, students solve various problems encountered during experiments to develop a further understanding of the theoretical knowledge and the principle of optics about the system. OMTOOLS offers the Young’s double-slit interference cage system kit for teaching or research use in a variety of optical laboratories. An OD 25.4 mm optic fiber collimator with FC/PC interfaces is included in the kit, and we also provide optional light sources. The system is compatible with your light sources and OD 25.4 mm optic fiber collimators. For optic fiber collimators with other outer dimensions such as 9 mm, 11 mm, 12 mm, 16 mm, and 18 mm, or other customized dimensions, we provide collimator adapters with SM1 threads. To facilitate the compatibility with adapters, we can replace the OMTF25A lens mounts with jack screws and fixed light sources with the OMTF25B lens mount with clamping rings free of charge. (Note: this kit only includes one optical double slit. See the slit specifications below if other slits are required)
Applicable system 30mmCoaxial cage system | material quality aluminum alloy |
Surface finishing Black anodic oxidation |
Fiber collimator with FC/PC interfaces, focal length 30 MM, collimating spot diameter 8.2 MM | 1 | PS1A25 stainless steel post | 1 |
OMGM0101 optical curtain | 1 | DVA081200 biconvex lens | 1 |
HPBC04503 aluminium alloy optical breadboard | 1 | OMTF25A 30 MM coaxial 3-axis reflection mirror mount | 1 |
OMJC8M6 fixed clamp mount | 1 | LDB30E 30 mm multi-purpose support holders | 2 |
Floor pad | 4 | PS1Z250 Ø6 MM stainless steel coaxial cage rod | 4 |
F2H30 30 mm XY lens t`ranslation mounts | 2 | Set screws | Several |
PSE25 Ø12 MM base sleeve | 1 | OMSF0303 optical double slit | 1 |
Note: this kit only includes one optical double slit. See the slit specifications below if other slits are required. |
OMTOOLS offers the Young’s double-slit interference cage system kit for teaching or research use in a variety of optical laboratories.
An OD 25.4 mm optic fiber collimator with FC/PC interfaces is included in the kit, and we also provide optional light sources.
The optical double slit sheet metals provided by OMTOOLS are machined from 300 stainless steel with a thickness of 30 μm. The double slit is mounted in a black anodizing Ø25.4 mm aluminium alloy housing, which can reduce the impact of reflection on the experiment to a greater extent. The double slit can be mounted in optical mounts with a diameter of 25.4 mm. The slit is available in a range of sizes for Young’s double-slit interference cage systems. The slits of different specifications lead to multiple sets of data.
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