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01 Newton’s Rings (1)

Aim

To show Newton’s rings.

Subjects

Diagram

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Figure 1:.

Equipment

Presentation

The prism is placed on the convex side of the 5000 mm5000 \mathrm{~mm}-lens. The camera looks almost perpendicular at a side of the prism (see Diagram). The image is projected. Concentric Newton’s rings are observed (see Figure 2).

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Figure 2:.

Explanation

Figure 3 shows the setup of the demonstration and the way the light rays go towards the camera (eye). The thin film between the flat and convex surface causes a phase difference between the two reflected rays: Reflection from the plane gives a phase change of Δϕ=0\Delta \phi=0 (the black ray); reflection from the convex surface gives a phase change of Δϕ=π\Delta \phi=\pi, and next to this phase change of π\pi the transit-time in the short air wedge adds to this phase difference (the red ray).

The incoming light is diffuse, so when the camera (eye) is shifted, another pair of interfering rays is caught by the camera, and a changed pattern is observed (see the black- and green colored ray in Figure 3).

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Figure 3:.

Using the 5000 mm5000 \mathrm{~mm}-lens makes the curvature in Figure 3 much less and so the layer of air will change much slower in the xx-direction, broadening the distance between the fringes.

Remarks

Sources