Decrease in intensity of light on undergoing successive reflections

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SUMMARY

The discussion addresses the intensity of light reflections from a thick plane mirror and the behavior of light from a long, thin cylindrical source. It confirms that the first image from a thick mirror is the brightest due to energy loss from scattering within the medium. Additionally, it clarifies that the intensity of light from a long cylindrical source is inversely proportional to the distance (r^(-1)), contrasting with the r^(-2) relationship of point sources. This distinction arises because a line can be viewed as a continuous series of point sources contributing to the observed light intensity.

PREREQUISITES
  • Understanding of light reflection and refraction principles
  • Familiarity with the concept of light intensity and its mathematical relationships
  • Knowledge of cylindrical light sources and their characteristics
  • Basic calculus for integrating light intensity over distance
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  • Study the principles of light scattering in dense media
  • Learn about the mathematical modeling of light intensity from line sources
  • Explore the differences between point sources and extended sources in optics
  • Investigate the effects of angle and orientation on light intensity measurements
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Physicists, optical engineers, and students studying light behavior and intensity distribution in various mediums.

Amith2006
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Sir,
1) A thick plane mirror shows a number of images of the filament of an electronic bulb. It is said that of these images the first image is the brightest. Is it true? If so, is it because some energy is lost in traversing through the dense medium?
2) It is said that the intensity of light at a large distance r from a long, thin cylindrical source of light is proportional to r^0. Is it true? I know that intensity of a point source is proportional to r^(-2). In what way is a long, thin cylindrical source of light different? Can't the cylindrical source be treated as a point source for large distances? Here the symbol ^ stands for power.
 
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1) Some light is scattered within the solid medium and at the interface of the solid and atmosphere. So some intensity (number of photons) is lost.

2) A line is essentially a continuous series of point sources, and each contributes to the light being received at some distance. If one does the integral, then one sees that the light intensity is inversely proportional to the distance r (or r-1) from the line.

Keep in mind this applies to a very long line, which is observed along a line perpendicular to the line of light sources.

If the line is short, then the intensity would approach that of a point source a long distance.

Also the orientation (angle) of the 'short' line with respect to the line of observation would have to be considered.
 

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