PHYSICS PROJECT REPORT ON PRISM WITH LIGHT RAY/LAWS OF REFLECTION

PHYSICS PROJECT REPORT ON PRISM WITH LIGHT RAY/LAWS OF REFLECTION

A plastic prism

In optics, a prism is a transparent optical element with flat, polished surfaces that refract light. At least two of the flat surfaces must have an angle between them. The exact angles between the surfaces depend on the application. The traditional geometrical shape is that of a triangular prism with a triangular base and rectangular sides, and in colloquial use “prism” usually refers to this type. Some types of optical prism are not in fact in the shape of geometric prisms. Prisms can be made from any material that is transparent to the wavelengths for which they are designed. Typical materials include glassplastic, and fluorite.

dispersive prism can be used to break light up into its constituent spectral colors (the colors of the rainbow). Furthermore, prisms can be used to reflect light, or to split light into components with different polarizations.

How prisms work

A triangular prism, dispersing light; waves shown to illustrate the differing wavelengths of light. (Click to view animation)

Light changes speed as it moves from one medium to another (for example, from air into the glass of the prism). This speed change causes the light to be refracted and to enter the new medium at a different angle (Huygens principle). The degree of bending of the light’s path depends on the angle that the incident beam of light makes with the surface, and on the ratio between the refractive indices of the two media (Snell’s law). The refractive index of many materials (such as glass) varies with the wavelength or color of the light used, a phenomenon known as dispersion. This causes light of different colors to be refracted differently and to leave the prism at different angles, creating an effect similar to a rainbow. This can be used to separate a beam of white light into its constituent spectrum of colors. A similar separation happens with iridescent materials, such as a soap bubble. Prisms will generally disperse light over a much larger frequency bandwidth than diffraction gratings, making them useful for broad-spectrum spectroscopy. Furthermore, prisms do not suffer from complications arising from overlapping spectral orders, which all gratings have.

Prisms are sometimes used for the internal reflection at the surfaces rather than for dispersion. If light inside the prism hits one of the surfaces at a sufficiently steep angle, total internal reflection occurs and all of the light is reflected. This makes a prism a useful substitute for a mirror in some situations.

Deviation angle and dispersion

A ray trace through a prism with apex angle α. Regions 0, 1, and 2 have indices of refraction {\displaystyle n_{0}}{\displaystyle n_{1}}, and {\displaystyle n_{2}}, and primed angles {\displaystyle \theta ‘} indicate the ray’s angle after refraction.

Ray angle deviation and dispersion through a prism can be determined by tracing a sample ray through the element and using Snell’s law at each interface. For the prism shown at right, the indicated angles are given by

{\displaystyle {\begin{aligned}\theta ‘_{0}&=\,{\text{arcsin}}{\Big (}{\frac {n_{0}}{n_{1}}}\,\sin \theta _{0}{\Big )}\\\theta _{1}&=\alpha -\theta ‘_{0}\\\theta ‘_{1}&=\,{\text{arcsin}}{\Big (}{\frac {n_{1}}{n_{2}}}\,\sin \theta _{1}{\Big )}\\\theta _{2}&=\theta ‘_{1}-\alpha \end{aligned}}}.

All angles are positive in the direction shown in the image. For a prism in air {\displaystyle n_{0}=n_{2}\simeq 1}. Defining {\displaystyle n=n_{1}}, the deviation angle {\displaystyle \delta } is given by

{\displaystyle \delta =\theta _{0}+\theta _{2}=\theta _{0}+{\text{arcsin}}{\Big (}n\,\sin {\Big [}\alpha -{\text{arcsin}}{\Big (}{\frac {1}{n}}\,\sin \theta _{0}{\Big )}{\Big ]}{\Big )}-\alpha }

If the angle of incidence {\displaystyle \theta _{0}} and prism apex angle {\displaystyle \alpha } are both small, {\displaystyle \sin \theta \approx \theta } and {\displaystyle {\text{arcsin}}x\approx x} if the angles are expressed in radians. This allows the nonlinear equation in the deviation angle {\displaystyle \delta } to be approximated by

{\displaystyle \delta \approx \theta _{0}-\alpha +{\Big (}n\,{\Big [}{\Big (}\alpha -{\frac {1}{n}}\,\theta _{0}{\Big )}{\Big ]}{\Big )}=\theta _{0}-\alpha +n\alpha -\theta _{0}=(n-1)\alpha \ .}

The deviation angle depends on wavelength through n, so for a thin prism the deviation angle varies with wavelength according to

{\displaystyle \delta (\lambda )\approx [n(\lambda )-1]\alpha }.

History

A triangular prism, dispersing light

Before Isaac Newton, it was believed that white light was colorless[citation needed], and that the prism itself produced the color. Newton’s experiments demonstrated that all the colors already existed in the light in a heterogeneous fashion, and that “corpuscles” (particles) of light were fanned out because particles with different colors traveled with different speeds through the prism. It was only later that Young and Fresnel combined Newton’s particle theory with Huygens’ wave theory to show that color is the visible manifestation of light’s wavelength.

Newton arrived at his conclusion by passing the red color from one prism through a second prism and found the color unchanged. From this, he concluded that the colors must already be present in the incoming light — thus, the prism did not create colors, but merely separated colors that are already there. He also used a lens and a second prism to recompose the spectrum back into white light. This experiment has become a classic example of the methodology introduced during the scientific revolution. The results of this experiment dramatically transformed the field of metaphysics, leading to John Locke‘s primary vs secondary quality distinction.[citation needed]

Newton discussed prism dispersion in great detail in his book Opticks.He also introduced the use of more than one prism to control dispersion.Newton’s description of his experiments on prism dispersion was qualitative, and is quite readable. A quantitative description of multiple-prism dispersion was not needed until multiple prism laser beam expanders were introduced in the 1980s

Types of prisms

Dispersive prisms

Comparison of the spectra obtained from a diffraction grating by diffraction (1), and a prism by refraction (2). Longer wavelengths (red) are diffracted more, but refracted less than shorter wavelengths (violet).

Dispersive prisms are used to break up light into its constituent spectral colors because the refractive index depends on frequency; the white light entering the prism is a mixture of different frequencies, each of which gets bent slightly differently. Blue light is slowed down more than red light and will therefore be bent more than red light.

Reflective prisms

Reflective prisms are used to reflect light, in order to flip, invert, rotate, deviate or displace the light beam. They are typically used to erect the image in binoculars or single-lens reflex cameras – without the prisms the image would be upside down for the user. Many reflective prisms use total internal reflection to achieve high reflectivity.

The most common reflective prisms are:

Beam-splitting prisms

Some reflective prisms are used for splitting a beam into two or more beams:

Polarizing prisms

There are also polarizing prisms which can split a beam of light into components of varying polarization. These are typically made of a birefringent crystalline material.

Deflecting prisms

Wedge prisms are used to deflect a beam of light by a fixed angle. A pair of such prisms can be used for beam steering; by rotating the prisms the beam can be deflected into any desired angle within a conical “field of regard”. The most commonly found implementation is a Risley prism pair. Two wedge prisms can also be used as an anamorphic pair to change the shape of a beam. This is used to make a round beam from the elliptical output of a laser diode.

Rhomboid prisms are used to laterally displace a beam of light without inverting the image.

Deck prisms were used on sailing ships to bring daylight below deck, since candles and kerosene lamps are a fire hazard on wooden ships.

In optometry

By shifting corrective lenses off axis, images seen through them can be displaced in the same way that a prism displaces images. Eye care professionals use prisms, as well as lenses off axis, to treat various orthoptics problems:

Prism spectacles with a single prism perform a relative displacement of the two eyes, thereby correcting eso-, exo, hyper- or hypotropia.

In contrast, spectacles with prisms of equal power for both eyes, called yoked prisms (also: conjugate prismsambient lenses or performance glasses) shift the visual field of both eyes to the same extent

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Physics Projects with Reports:

  1. TO CONSTRUCT A CIRCUIT FOR TOUCH ALARM.
  2. EDDY CURRENT {WITHOUT MODEL }
  3. PHOTOCONDUCTIVE CELL
  4. MUTUAL INDUCTION
  5. TO STUDY NPN-TRANSISTOR AMPLIFIER
  6. TO CONSTRUCT A ELECTRIC MOTORS (D.C.MOTOR)
  7. TO STUDY HOW A TRANSISTOR AMPLIFIER WORK ‘PNP’ AMPLIFIER TRANSISTOR.
  8. HOUSEHOLD CIRCUITS
  9. AC TO DC CONVERTER (FULL WAVE RECTIFIER)
  10. AC TO DC CONVERTER (HALF WAVE RECTIFIER)
  11. TO CONSTRUCT A CIRCUIT OF FENCE WIRE BURGLAR ALARM
  12. TO SHOW THE PRINCIPLE OF FARADAY’S AND A.C. GENERATOR.
  13. THERMOCOUPLE
  14. TO STUDY FARADAY’S LAWS-TO FIND THE CHARGE ON AN ELECTRON
  15. FARADAY’S LAW’S OF ELECTROLYSIS
  16. TO STUDY A POSITIVE FEED BACK CIRCUIT OF AN AUDIO OSCILLATOR (LC OSCILLATOR)
  17. HOW DOES AN ELECTRIC GENERATOR WORK
  18. TO SHOW THAT A SOLENOID CARRYING AN ELECTRIC CURRENT PRODUCES A MAGNETIC FIELD SIMILAR TO THAT PRODUCED BY A BAR MAGNET.
  19. ELECTROCHEMICAL CELL (PRIMARY CELL)
  20. BOOLAN LOGIC GATE
  21. TO STUDY THE CHARGE AND DISCHARGING OF CAPACITOR IN SERIES
  22. WORKING OF POTENTIOMETER
  23. KIRCHOFF’S LAW
  24. TO DEMONSTRATE THE WORKING OF AN ELECTROLYTIC CAPACITOR BY MEANS OF ITS CHARGING AND DISCHARGING WITH THE HELP OF AN AUDIO OSCILLATOR AND TO STUDY AND COMPARE THE TWO CAPACITORS UNDER SERIES AND PARALLEL COMBINATION.(Z)
  25. RADIOACTIVITY AND NUCLEAR REACTIONS.
  26. RADIOISOTOPE THERMOELECTRIC GENERATOR.
  27. TO CONSTRUCT A CIRCUIT OF SOUND OPERATED SWITCH.
  28. TO CONSTRUCT A CIRCUIT OF TIME OPERATED SWITCH.
  29. TO CONSTRUCT A CIRCUIT OF SOUND AMPLIFIER.
  30. TO CONSTRUCT A CIRCUIT OF A FIRE ALARM.
  31. TO CONSTRUCT A CIRCUIT OF CLAP SWITCH.
  32. TO CONSTRUCT A CIRCUIT OF TRANSISTOR SWITCH
  33. TO FIND OUT OPTICAL ACTIVITY ARISES WHEN THE POLARIZATION AXIS OF LIGHT IS ROTATED AS IT PASSES THROUGH A SUBSTANCE
  34. PUSH-PULL AMPLIFIER
  35. HARTLEY OSCILLATORS
  36. PUSH PULL AMPLIFIER
  37. REPORT ON MAGNETIC FIELDS, MAGNETIC FORCES, AND ELECTROMAGNETIC INDUCTION LAWS OF REFRACTION (Z).
  38. RAY OPTICS-TO FIND REFRACTIVE INDEX OF THE MATERIAL OF THE PRISM BY TOTAL INTERNAL REFRACTION (Z).
  39. TO DEMONSTRATE THE WORKING OF AN ELECTROLYTIC CAPACITOR BY MEANS OF ITS CHARGING AND DISCHARGING WITH THE HELP OF AN AUDIO OSCILLATOR AND TO STUDY AND COMPARE THE TWO CAPACITORS UNDER SERIES AND PARALLEL COMBINATIONS.
  40. TO STUDY THE EFFECT OF THE DIAMETER AND THE NUMBER OF TURNS OF THE SPRING ON ITS STRENGTH HAS BEEN INVESTIGATION IN THIS STUDY.(Z)
  41. TO FIND OUT THE THERMAL COEFFICIENT OF RESISTANCE FOR A DIVAN SET OF WIRES AND THUS SUGGEST THE WIRE IN WHICH ENERGY LOSS DUE TO HEAT GENERATION IS MINIMUN.(Z)
  42. TO SEE THAT WATER CONDUCTS ELECTRICITY BETTER WHEN IMPURITIES ARE ADDED IT. (Z)
  43. TO MAKE NOR GATE WITH THE COMBINATION OF TWO GATES. (Z)
  44. PASCAL’S LAW AND ITS APPLICATIONS
  45. BRIDGE RECTIFIER- A CIRCUIT USING FOUR DIODES TO PROVIDE FULL WAVE RECTIFICATION.CONVERTS AN AC VOLTAGE TO A PULSATING DC VOLTAGE.
  46. TO CONSTRUCT A CIRCUIT OF QUIZ BUZZER.
  47. TO CONSTRUCT A CIRCUIT OF LASER SECURITY SYSTEM.
  48. TO CONSTRUCT A CIRCUIT OF RAIN ALARM.
  49. TO CONSTRUCT A CIRCUIT OF WATER LEVEL INDICATOR.
  50. THE EFFECT OF TEMPERATURE ON DISPOSABLE AND NON DISPOSABLE BATTERIES
  51. TO INVESTIGATE THE EFFECT OF THE FOLLOWING FACTORS ON THE INTERNAL RESISTANCE OF A LACLANCHE CELL.
  52. TO CONSTRUCT A CIRCUIT OF OPTICAL SWITCHING.
  53. TO CONSTRUCT A CIRCUIT OFCAPACITOR CHARGE OSCILATOR
  54. TO CONSTRUCT A CIRCUIT OFCAPACITOR STORAGE LED
  55. TO CONSTRUCT A CIRCUIT OF TWO TRANSISTOR OSCILLATOR
  56. EXPERIMENTS IN ELECTROCHEMISTRY
  57. TO SHOW THE UNIDIRECTION ACTION OF DIODE
  58. OPTICAL FIBER COMMUNICATION
  59. TO CONSTRUCT A CIRCUIT OF ELECTRONIC EYE

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