1. ABERRATIONS Lecturer in PHYSICS Silver Jubilee Govt.,College(A),
Dr.N. LALITHA KUMARI
Lecturer in PHYSICS
Silver Jubilee Govt.,College(A),
KURNOOL

2. ABOUT LENS C F2 F1 R1 R2 f

3. 1 2 2 1
1---marginal rays 2----paraxial rays.

4. Derivation produced by a thin lensβ α δ c o I u v
From the ▲AIO, δ=α+β
Hence α=tanα and β=tanβ
α= h/u and β=h/v
Now, δ=h/u + h/v since u=-ve and v=+ve
δ=h/v-h/u=h(1/v-1/u)
Or δ=h/f

5. ABERRATIONS Definition of Aberrations. Types of Aberrations.
Chromatic Aberrations.
Monochromatic Aberrations.
Mathematical Analysis & Visuals.
Methods of Elimination.

6. What is an Aberration?
The deviations or defects observed in the actual size, position, shape and colour in the image of an object formed by a single lens are called Aberrations.

7. CAUSE FOR ABERRATIONS These aberrations are caused due to
the convergence of different rays to
different points.

8. TYPES OF ABERRATIONS

9. CHROMATIC ABERRATIONS
Formation of Multicoloured image.
Disability of lens to converge different colours at different points.

10. TYPES OF CHROMATIC ABERRATIONS
Longitudinal
The formation of images of different colours in different positions along the axis
Lateral /Transverse
The defect in images of different colours are formed of different sizes perpendicular to the axis .

11. LONGITUDINAL CHROMATIC ABERRATIONS
Chromatic aberration of a single lens causes different wavelengths of light to have differing focal lengths.
L.C.A.= f r - f v

12. CALCUALTION OF LONFITUDINAL CHROMATIC ABERRATION OF A THIN LENS
When the object is situated at infinity.
When the object is situated at a finite distance.

13. When the object is situated at infinity
General formulae=
1/f=(µ-1)(1/R1-1/R2),
If fv,fR and fy be the focal length of the lens for violet, red and yellow
1/fv=(µv-1)(1/R1-1/R2), ………..(1)
1/fR=(µR-1)(1/R1-1/R2),……………(2)
1/fY=(µY-1)(1/R1-1/R2)……………….(3)
2 in 1 gives 1/fv-1/fR=(µv-µR)(1/R1-1/R2),
fR-fv =(µv-µR)(µy-1)(1/R1-1/R2),
fv.fR (µy-1)
BY SOLVING THEM
fR-fv=ώ.fy
WHEN THE IMAGE AT A FINITE DISTANCE THEN
VR-VV=ώ/fV .Vy2

14. LATERAL/TRANSVERSE CHROMATIC ABERRATIONS
Origin of transverse chromatic aberration. The size of the image varies from one color to the next.

15. Visual of chromatic aberrations1

16. VISUAL FOR CHROMATIC ABERRATION 2
Severe purple fringing can be seen at the edges of the horse's forelock, mane, and ear.

17. VISUAL FOR CHROMATIC ABERRATION 3
On top is corner detail in a photograph taken with a higher quality lens; bottom is a similar photograph taken with a wide angle lens showing visible chromatic aberration (especially at the dark edges on the right).

18. VISUAL 4 A cross made by two black match stick mounted on a cork.

19. Methods of elimination of chromatic aberration
Achromatic Doublet
A combination of convex lens made up of
by crown glass and concave lens made up of
by flint glass.
Arranging two converging lenses coaxially
Two convex lenses made up of by same
material arranged coaxially at a distance of
d = f1+f2 2

20. ACHROMATIC DOUBLET
For an achromatic doublet, visible wavelengths have approximately the same focal length.
Diffractive optical element with complementary dispersion properties to that of glass can be used to correct for color aberration.

21. USING TWO CONVEX LENSES
If the distance between the lenses is
d = f1+f2 2

22. MONOCHROMATIC ABERRATIONS
The deviations in the actual size, shape and position in the image of an object formed by a single lens, when the object is illuminated by single wavelength light.

23. TYPES OF MONO CHROMATIC ABERRATION
Spherical Aberrations.
Astigmatism.
Coma.
Distortion.
Curvature.

24. SPHERICAL ABERRATION
Def. : The failure or inability of the lens to form a point image of an axial point object.
TYPES :
Longitudinal : the formation of image in different positions along the axis
Lateral : the formation of image in different sizes perpendicular to the axis.

25. VISUAL OF LONGITUDINAL SPHERICAL ABERRATION
Side view and chromatic Airy disc of a bright star at image plan. An asymmetry variation of the Airy disk occurs around the paraxial focal plane, displaying spherical aberrations

26. METHODS OF ELIMINATION OF SPHERICAL ABERRATION
By means of stops.
By using two suitable lenses in contact.
By using crossed lens.
By using two plano – convex lenses separated by a distance.

27. ASTIGMATISM
When a point object is situated far of the axis of a lens, the image formed by the lens is not in a perfect focus.
It consists two mutually perpendicular lines separated by finite distance.
Side view and Airy disc of a bright star coming 25° off axis showing astigmatism; the tangential and sagittal line image do not coincide in the area of less conSide view and Airy disc of a bright star coming 25° off axis showing astigmatism; the tangential and sagittal line image do not coincide in the area of less confusion and in this case display a cross shape.
fusion and in this case display a cross shape

28. Astigmatism as evidenced by the blurring of white dots.
VISUAL OF ASTIGMATISM
Astigmatism as evidenced by the blurring of white dots.

29. Spoked wheel
.Classic example of astigmatism. Left wheel: no astigmatism. In the presence of astigmatism (middle and right wheels) one discriminates between the sagittal and tangential foci.

30. ELIMINATION OF SPHERICAL ABERRATIONS
By using two convex
Lenses coaxially at a distance
d = f1 – f2
d = f1 – f2

31. ELIMINATION OF ASTIGMATISM
USING ANASTIGMAT
By using a convex and a concave lens of suitable focal lenghs and separated by a distance . Such a combination is called an anastigmat.

32. COMA, "comet" in latin
Coma occurs because off-axis rays no not quite converge at the focal plane. Coma is positive when off-axis rays focus furthest from the axis, and negative when they are closest.
spot diagram showing coma aberration. The resulting image takes the shape of a comet.

33. ELIMINATION OF COMA using stops Abbe condition µ1Y1SinӨ1 = µ2Y2SinӨ2
Using Aplanatic surface

34. DISTORTION
The variation in the magnifications produced by a lens for different axial distances results in an aberration called distortion.
It is of two types.
1.Pin cushion .
2.Barrel shaped.

35. ORIGIN FOR DISTORTION
The influence of stop position on distortion. Note that the image size h differs for a constant object size y.

36. ELIMINATION OF DISTORTION
A stop is placed in between two symmetrical lenses, so that the pin – cushion distortion produced by the first lens is compensated by the barrel – shaped distortion produced by the second lens.

37. VISUAL FOR DISTORTION 1

38. VISUAL FOR DISTORTION 2
Geometric distortion: the photograph does not flatter the person at the left. (18-mm lens on a 24×36 mm slide)

39. curvature
The image of an extended plane object due to a single lens is not flat one but will be a curved surface. The central portion of the image nearer the axis is in focus but outer regions of the image away from the axis are blurred.

40. CURVATURE OF THE FIELD DUE TO CONVEX LENS

41. CURVATURE DUE TO CONCAVE LENS

42. ELIMINATION OF CURVATURE

43. THANK U