Newton's rings are ring-shaped interference maximum and
minimum seeming around the point of tang ency of a marginally curved convex lens
and a plane-parallel plate as light permits through the lens and plate.
The interference pattern in the form of rings happens when
light is mirrored from two surfaces, one of which is flat, and the other has a moderately
large radius of curvature and comes into contact. If a beam of homo chromatic
light is event on such a system in a direction erect to the plane surface, then
the light waves reflected from each of these surfaces interfere with each
other. The interference pattern shaped in this way comprises of the surfaces of
a dark circle witnessed in the place of contact and the neighboring light and
dark concentric rings surrounding it.
The classical description of the phenomenon:
In the time of Newton, because of a lack of evidence on the
nature of light, it was awfully difficult to give a full explanation of the
mechanism of the appearance of rings. Newton outmoded a connection between the
dimensions of the rings and the curvature of the lens; He understood that the detected
effect was connected to the periodicity of light, but it was only later that
Thomas Young could satisfactorily clarify the reasons for the formation of the
rings. Let us follow the course of his reasoning. They are based on the postulation
that light is waves . Let us consider the case when a monochromatic wave falls
almost perpendicularly to a plane-convex lens.
Wave 1 appears as a result of reflection from the convex
surface of the lens at the glass-air interface, and wave 2 appears as a result
of reflection from the plate at the air-glass interface. These waves are
coherent , that is, they have the same wavelengths, and the phase difference is
constant. The phase difference arises from the fact that wave 2
permits a larger path than wave 1. If the second wave lags
behind the first by an integer number of wavelengths, then, folding, the waves
amplify each other.
On the contrary, if the second wave lags behind the first by
an odd number of half-waves, then the vacillations caused by them will occur in
opposite phases, and the waves cancel each other.
In order to take into account the fact that in different materials
the speed of light is different, when influential the positions of minimum and maximum use not the path difference, but the optical path change.
If the radius of curvature R of the lens surface is known,
then it is possible to calculate at which distances from the point of contact
of the lens with the glass plate the path differences are such that waves of a
certain length λ cancel each other. These distances are the radii of the dark
rings of Newton.
Usage
Newton's rings are used to measure the radii of curving of
surfaces, to measure wavelengths of light and refractive indices. Newton's
rings are an unwanted phenomenon.
Used in physiology. Counting of the shaped rudiments is made
after grinding the cover glass and the Goriaev chamber before the appearance of
Newton's rings.


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