Optical Image Formation: Principles and Conditions

Image formation with broad
bundles of rays
LL2 section 57
Image formation with broad bundles of rays is only possible for special optical systems
Suppose all rays starting from O that travel through the optical system intersect again
at O’.
Wave surfaces near O for rays passing through O are spheres.  Same for O’.
Wave surfaces are surfaces of constant phase.
The 
change in phase
 along different rays between points of intersection with two
given wave surfaces is the same.
The 
total change in phase
 between the points O and O’ is the same for the different
rays.
The 
optical path length 
 is the same for all these rays.
Conditions for imaging a line
segment using broad beams.
Optical path length of all
rays that start from O and
end at O’.
(not the same 

’ measured from
principal points as in sec 56.)
 and 
’ axes need not be parallel to each other or to the optical axis.
Magnification
Ratio of length elements for image and object.
Constant along a sufficiently small line element
Negative cosine of angle between direction of ray and x axis.
(see (55.2) and following.
The optical path length 
 + d
 for all rays starting from point d
 and arriving
at point d
’ must be the same.
This is the condition that the paths of rays in the
optical system must satisfy to have image formation
for a small line segment using broad beams.
It must be fulfilled for all rays staring from O.
Image formation by axially-symmetric optical system.
Take object to be a line
segment on the optical axis.
Image is also on
optical axis by axial
symmetry.
A ray approaching the optical system along the optical axis has n
x
 = 1.
Afterwards, n
x
’ = 1 by symmetry, i.e. it is undeflected.
For these rays
General condition of image formation
A specific direction of line segment
Specific case of axial symmetry
Condition for image formation
Line segment dr     
Object is a small portion of a
plane perpendicular to the
optical axis.
Image is also perpendicular
to the axis.
Next consider perpendicular line segment.
For arbitrary segment dy in plane to be imaged,
General condition for imaging
For specific line segment
perpendicular to optical axis.
Rays emerging from intersection of object plane with optical axis
with 
 = 0 are undeflected due to assumed axial symmetry: 
’ = 0.
Then for non-zero angles, the condition for imaging of transverse planes is
Imaging of 3D object using broad beams is impossible
even for small volumes because the conditions for
longitudinal and transverse imaging
are incompatible.
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Understanding the principles and conditions governing optical image formation, including the role of broad bundles of rays, wave surfaces, magnification ratios, and axially-symmetric optical systems. Explore the conditions for imaging line segments, optical path lengths, and the general criteria for image formation in various scenarios.

  • Optical Image Formation
  • Principles
  • Conditions
  • Magnification
  • Axially-Symmetric

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  1. Image formation with broad bundles of rays LL2 section 57

  2. Image formation with broad bundles of rays is only possible for special optical systems Suppose all rays starting from O that travel through the optical system intersect again at O . Wave surfaces near O for rays passing through O are spheres. Same for O . Wave surfaces are surfaces of constant phase. The change in phase along different rays between points of intersection with two given wave surfaces is the same. The total change in phasebetween the points O and O is the same for the different rays. The optical path length is the same for all these rays.

  3. Conditions for imaging a line segment using broad beams. Optical path length of all rays that start from O and end at O . (not the same measured from principal points as in sec 56.) and axes need not be parallel to each other or to the optical axis.

  4. Magnification Ratio of length elements for image and object. Constant along a sufficiently small line element Negative cosine of angle between direction of ray and x axis. (see (55.2) and following.

  5. The optical path length + d for all rays starting from point d and arriving at point d must be the same. This is the condition that the paths of rays in the optical system must satisfy to have image formation for a small line segment using broad beams. It must be fulfilled for all rays staring from O.

  6. Image formation by axially-symmetric optical system. Take object to be a line segment on the optical axis. Image is also on optical axis by axial symmetry. A ray approaching the optical system along the optical axis has nx = 1. Afterwards, nx = 1 by symmetry, i.e. it is undeflected.

  7. For these rays General condition of image formation A specific direction of line segment Specific case of axial symmetry

  8. Condition for image formation

  9. Next consider perpendicular line segment. Line segment dr Image is also perpendicular to the axis. Object is a small portion of a plane perpendicular to the optical axis.

  10. For arbitrary segment dy in plane to be imaged, General condition for imaging For specific line segment perpendicular to optical axis.

  11. Rays emerging from intersection of object plane with optical axis with = 0 are undeflected due to assumed axial symmetry: = 0. Then for non-zero angles, the condition for imaging of transverse planes is

  12. Imaging of 3D object using broad beams is impossible even for small volumes because the conditions for longitudinal and transverse imaging are incompatible.

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