User:Epzcaw/Classical Optics

Classical optics

Classical optics is divided into two main branches: geometrical optics and physical optics. In geometrical, or ray optics, light is considered to travel in straight lines, and in physical, or wave optics, light is considered to be an electromagnetic wave.

Geometrical optics can be viewed as an approximation of physical optics which can be applied the wavelength of the light used is much smaller than the size of the optical elements or system being modelled.

Geometrical optics

Geometrical optics, or ray optics, describes the propagation of light in terms of "rays" which travel in straight lines, and whose paths are governed by the laws of reflection and refraction at interfaces between different media.^[1] These laws were discovered empirically as far back as 984AD ^[2] and have been used in the design of optical components and instruments from then until the present day. They can be summarised as follows:

When a ray of light hits the boundary between two transparent materials, it is divided into a reflected and a refracted ray.

The law of reflection says that the reflected ray lies in the plane of incidence, and the angle of reflection equals the angle of incidence.

The law of refraction says that the refracted ray lies in the plane of incidence, and the sine of the angle of refraction divided by the sine of the angle of incidence is a constant.

{\frac {\sin {\theta _{1}}}{\sin {\theta _{2}}}}=n

where $n$ is a constant for any two materials and a given colour of light. It is known as the refractive index.

The laws of reflection and refraction can be derived from Fermat's principle which states that the path taken between two points by a ray of light is the path that can be traversed in the least time.^[3]

Stuff from existing Optics article

Physical optics

In physical optics, light is considered to propagate as a wave. This model predicts phenomena such as interference and diffraction which are not explained by geometric optics. The speed of light waves is approximately 3.10 ⁸ m/s. The wavelength of visible light waves varies between 400-700nm but light waves are usually considered to also include infrared waves (0.7-300μm) and ultraviolet waves (10-400nm).

The wave model can be used to make predictions about how an optical system will behave without requiring an explanation of what is "waving" in what medium. Until the middle of the 19th century, most physicists believed in an "ethereal" medium in which the light distubrance propagated.^[4] The existence of electromagnetic waves was predicted in 1865 by Maxwell's equations. These waves propagate at the speed of light and have varying electric and magnetic fields which are orthogonal to one another, and also to the direction of propagation of the waves.^[5] Light waves are now generally treated as electromagnetic waves except when quantum mechanical effects have to be considered.

Modelling and design of optical systems

Many simplifed approximations are available for analysing and designing optical systems. Most of these use a single scalar quantity to represent the electric field of the light wave, rather than using a vector model with orthogonal electric and magnetic vectors.^[6] TheHuygens–Fresnel equation is one such model. This was derived empirically by Fresnel in 1815, based on Huygen's hypothesis that each point on a wavefront generates a secondary spherical wavefront, which Fresnel combined with the principle of superposition of waves. The Kirchoff diffraction equation, which is derived using Maxwell's equations, puts the Huygens-Fresnel equation on a firmer physical foundation. Examples of the application of Huygens–Fresnel principle can be found in the sections on diffraction and Fraunhofer diffraction.

More rigorous models, involving the modelling of both electric and magnetic fields of the light wave, are required when dealing with the detailed interaction of light with materials where the interaction depends on their electric and magnetic properties. For instance, the behaviour of a light wave interacting with a metal surface is quite different from what happens when it interacts with a di-electric material. A vector model must also be used to model polarized light.

Numerical modeling techniques such as the Finite element method, the Boundary element method and the Transmission-line matrix method can be used to model the propagation of light in systems which cannot be solved analytically. Such models are computationally demanding and are normally only used to solve small-scale problems that require accuracy beyond that which can be achieved with analytical solutions.^[7]

All of the results from geometrical optics can be recovered using the techniques of Fourier optics which apply many of the same mathematical and analytical techniques used in acoustic engineering and signal processing.

Gaussian beam propagation is a simple paraxial physical optics model for the propagation of coherent radiation such as laser beams. This technique partially accounts for diffraction, allowing accurate calculations of the rate at which a laser beam expands with distance, and the minimum size to which the beam can be focused. Gaussian beam propagation thus bridges the gap between geometric and physical optics.^[8]

Stuff from existing Optics article

Relationship between geometric and physical optics

The "ray" in geometric optics is an abstraction that can be used to predict the path of light. A light ray is a ray that is perpendicular to the light's wavefronts (and therefore collinear with the wave vector). Light rays bend at the interface between two dissimilar media and may be curved in a medium in which the refractive index changes. Geometrical optics provides rules for propagating these rays through an optical system, which indicates how the actual wavefront will propagate. This is a significant simplification of optics that fails to account for optical effects such as diffraction and polarization. It is a good approximation, however, when the wavelength is very small compared with the size of structures with which the light interacts and is still the main method used for designing lenses. Geometric optics can be used to describe the geometrical aspects of imaging, including optical aberrations.

References

^ Lipson, Lipson & Lipson, 2011, 4th Edition, Cambridge University Press, p48
^ Rashed, Roshdi (1990). "A pioneer in anaclastics: Ibn Sahl on burning mirrors and lenses". Isis 81 (3): 464–491. doi:10.1086/355456
^ Arthur Schuster, An Introduction to the Theory of Optics, London: Edward Arnold, 1904 online.
^ MV Klein & TE Furtak, 1986, Optics, John Wiley & Sons, New York
^ Maxwell, James Clerk (1865). "A dynamical theory of the electromagnetic field" (pdf). Philosophical Transactions of the Royal Society of London. 155: 499. This article accompanied a December 8, 1864 presentation by Maxwell to the Royal Society. See also A dynamical theory of the electromagnetic field.
^ M. Born and E. Wolf (1999). Principle of Optics. Cambridge: Cambridge University Press. ISBN 0521642221.
^ J. Goodman (2005). Introduction to Fourier Optics (3rd ed, ed.). Roberts & Co Publishers. ISBN 0974707724.{{cite book}}: CS1 maint: extra punctuation (link)
^ A. E. Siegman (1986). Lasers. University Science Books. ISBN 0935702113. Chapter 16.

[1] Lipson, Lipson & Lipson, 2011, 4th Edition, Cambridge University Press, p48

[2] Rashed, Roshdi (1990). "A pioneer in anaclastics: Ibn Sahl on burning mirrors and lenses". Isis 81 (3): 464–491. doi:10.1086/355456

[3] Arthur Schuster, An Introduction to the Theory of Optics, London: Edward Arnold, 1904 online.

[4] MV Klein & TE Furtak, 1986, Optics, John Wiley & Sons, New York

[5] Maxwell, James Clerk (1865). "A dynamical theory of the electromagnetic field" (pdf). Philosophical Transactions of the Royal Society of London. 155: 499. This article accompanied a December 8, 1864 presentation by Maxwell to the Royal Society. See also A dynamical theory of the electromagnetic field.

[Born_and_Wolf-6] M. Born and E. Wolf (1999). Principle of Optics. Cambridge: Cambridge University Press. ISBN 0521642221.

[7] J. Goodman (2005). Introduction to Fourier Optics (3rd ed, ed.). Roberts & Co Publishers. ISBN 0974707724.{{cite book}}: CS1 maint: extra punctuation (link)

[8] A. E. Siegman (1986). Lasers. University Science Books. ISBN 0935702113. Chapter 16.

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