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# Cylindrical Lens: Cylindrical lens is a section of a cylindrical rod.

Cylindrical Lenses and Astigmatism. Cylindrical Lens: Cylindrical lens is a section of a cylindrical rod. One surface is cylindrical while the opposite is plane. Cylindrical Lenses and Astigmatism. Power of thin lens:. s. s . Cylindrical Lenses and Astigmatism.

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## Cylindrical Lens: Cylindrical lens is a section of a cylindrical rod.

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1. Cylindrical Lenses and Astigmatism Cylindrical Lens: Cylindrical lens is a section of a cylindrical rod. One surface is cylindrical while the opposite is plane. Optics 1----by Dr.H.Huang, Department of Applied Physics

2. Cylindrical Lenses and Astigmatism Power of thin lens: s s Optics 1----by Dr.H.Huang, Department of Applied Physics

3. Cylindrical Lenses and Astigmatism Example: A thin plano-cylindrical lens in air has a radius of curvature of 10 cm, a refractive index of 1.50 and an axial length of 5 cm. Light from a point object is incident on the convex, cylindrical surface from a distance of 25 cm to the left of the lens. Find the position and length of the line image formed by the lens. Solution: Object vergence S=1/s= 1/(0.25) = 4.0 D Power of lens P=(n2n1)/R= (1.51)/0.1= 0.5/0.1= +5.0 D Image vergence S=S+P=1.0 D, so s=1/S=1.0 m to the right of the lens. The line image length Example: A thin, cylindrical lens of +10.0 D power and a vertical cylinder axis is located 25 cm from a point source of light. A square aperture 1 cm on a side is placed directly in front of the lens. (a) Describe the image of the point source formed by the lens. (b) Describe the light pattern on a screen positioned halfway between lens and line image. Solution: (a) Object vergence S=1/s=1/(0.25) = 4.0 D, Image vergence S=S+P=+6.0 D, so s=1/S= 0.167 m to the right of the lens. Line image length (b) Screen at x=s/2=8.35 cm. Height: width: Optics 1----by Dr.H.Huang, Department of Applied Physics

4. Cylindrical Lenses and Astigmatism Power Cross: An astigmatic eye, while possesses predominately spherical optics, might have a cylindrical lens component whose axis can be in any direction. Convention: angles are measured counterclockwise from the positive x-axis. The coordinate system is the one seen by the examiner, not by the patient. use 180 instead of 0 to avoid confusion with zero power @ can also be used to replace X Optics 1----by Dr.H.Huang, Department of Applied Physics

5. Cylindrical Lenses and Astigmatism Combining Cylindrical Powers: Two cylindrical lens in contact: powers along parallel axes simply add algebraically and powers along perpendicular axes remain independent of one another. circular aperture square aperture interval of Sturm conoid of Sturm circle of least confusion: the nearest approximation to a focused image conjugate to a point object. Optics 1----by Dr.H.Huang, Department of Applied Physics

6. Cylindrical Lenses and Astigmatism Example: Let a composite cylindrical lens have perpendicular powers of +6.0180 and +7.090. A point object is situated at 50 cm from the lens. Line images then form as follows: A vertical line due to the +7.0 D power and a horizontal line image due to the +6.0 D power. Assume a circular aperture of 4.0 mm diameter (Under bright lighting conditions this is roughly the diameter of the pupil of the eye, which serves as the limiting aperture for the eye.). Determine the lengths of the two line images and describe the circle of least confusion. Solution: Object vergence: S=1/s=1/(0.5)=2.0 D vertical line image vergence S1=S+P1=2+7=+5.0 D, so s1=1/S1=0.20 m horizontal line image vergence S2=S+P2=2+6=+4.0 D, so s2=1/S2=0.25 m s s1 s s2 Optics 1----by Dr.H.Huang, Department of Applied Physics

7. Cylindrical Lenses and Astigmatism Example: What combination of a spherical and a cylindrical lens produces a lens with vertical power axis of +10.0 D and horizontal power axis of +3.0 D? Solution: The cylindrical lens may have one axis at zero power while the spherical lens must have identical powers along both axes. Optics 1----by Dr.H.Huang, Department of Applied Physics

8. Cylindrical Lenses and Astigmatism Example: Consider a toric lens whose two surfaces are spherical and toroidal. The spherical side has a power of +6.0 D, while the toroidal side is described by 4.045/2.0135. Determine (a) the power cross of the lens, and (b) the interval of Sturm for a point object at 50 cm from the lens. Solution: Object vergence S=1/s=1/(0.5)=2.0 D The +4.0 D power produces an image vergence of +2.0 D and the image distance is 50 cm. Image is tilted at 135 from the horizontal. The +10 D power produces an image vergence of +8.0 D and the image distance is 12.5 cm. Image is tilted at 45 from the horizontal. The interval of Sturm is 37.5 cm. A toroid with two circular cross sections of radii r1 and r2. Optics 1----by Dr.H.Huang, Department of Applied Physics

9. Cylindrical Lenses and Astigmatism Ocular Astigmatism: Astimagtism occurs in the eye due to an additional cylindrical curvature in addition to the spherical curvature. The correction can be made in the form of a sphero-cylindrical prescription. Example: Consider a “reduced eye”, that is, one whose optical behavior is well-approximated by refraction at a single surface at the cornea, separating air from the vitreous fluid of refractive index 4/3. The axial length of this eye is 24.24 mm and its measured powers along the vertical and horizontal axes are +59 D ad +57 D, respectively. What spectacle correction is required for good, distant vision if the correcting lens is to be 12 mm in front of the cornea? Solution: To form an image of a distant object on retina, S=n/s=+55.0 D The contact lens correction power at the cornea should be: CP90=5559=4.0 D CP180=5557=2.0 D Suppose the spectacle powers to be SP, since we obtain SP90=4.20 D and SP180=2.05 D. There are two combinations of a spherical and cylindrical surface to result in this correction. In standard notation, they are 2.05/2.15180 and 4.20/+2.1590. Optics 1----by Dr.H.Huang, Department of Applied Physics

10. Cylindrical Lenses and Astigmatism Classification of astigmatism in an unaccommodated eye: Assume the astigmatic line images are along horizontal and vertical axes and the vertical line image results from the stronger convergence. (a) CMA (compound myopic astigmatism): both lines images fall short of retina (b) SMA (simple myopic astigmatism): horizontal line image on retina (c) MXA (mixed astigmatism): retina between two line images (d) SHA (simple hyperopic astigmatism): vertical line image on retina (e) CHA (compound hyperopic astigmatism): both line images beyond retina a SHA eye looking at H a SMA eye looking at H Optics 1----by Dr.H.Huang, Department of Applied Physics

11. Cylindrical Lenses and Astigmatism • Homework: • Light rays emanating in air from a point object on axis strike a plano-cylindrical lens with its convex surface facing the object. Describe the line image by length and location if the lens has a radius of curvature of 5 cm, a refractive index of 1.60, and an axial length of 7 cm. The point object is 15 cm from the lens. • A plano-cylindrical lens in air has a radius of curvature of 10 cm, a refractive index of 1.50, and an axial length of 5 cm. Light from a point object is incident on the concave, cylindrical surface from a distance of 25 cm to the left of the lens. Find the position and length of the line image formed by the lens. • Determine the interval of Sturm for a composite cylindrical lens with perpendicularly oriented powers, given by +5.0090 and +10.00180, when the lens is illuminated by rays of light from a point source object at 30.00 cm from the lens. A circular aperture of 1.00 cm diameter is positioned at the lens. Also describe the circle of least confusion. • What combination of a spherical and a cylindrical lens produces a composite lens with vertical power axis of +6.00 D and horizontal power axis of +2.00 D? • One side of a lens is spherical with a power of +8.00 D, and the other side is toric, described by +3.00/5.00120. Determine the power cross and Sturm interval of the lens for a point object 40 cm from the lens. Optics 1----by Dr.H.Huang, Department of Applied Physics

12. Aberration Introduction: Aberration:departure of an image from perfection Chromatic Aberration:variation of the refractive index of a material with wavelength Monochromatic Aberrations: deviation even if monochromatic Classification of Aberrations: 1(a). Due to the material of the lens (chromatic aberrations) LCA: longitudinal chromatic aberrations TCA: transverse chromatic aberrations 1(b). Due to the form of the lens (monochromatic aberrations) S: spherical aberration C: coma A: oblique astigmatism P: curvature of field (Petzval curvature) D: distortion 2(a). Axial aberrations—axial object points only S; LCA 2(b). Oblique aberrations—off-axis objects points only TCA; C; A; P; D Optics 1----by Dr.H.Huang, Department of Applied Physics

13. Aberration Chromatic Aberrations: LCA LCA is the axial (longitudinal) distance between two focal points for a given wavelength range. Chromatic Aberrations: TCA Linear TCA: the difference between the size of the image in red (C) and blue (F) light. Angular TCA: the angle  between the emerged red and blue rays. chromatic aberration of the eye Optics 1----by Dr.H.Huang, Department of Applied Physics

14. Aberration Achromatic Doublet Optics 1----by Dr.H.Huang, Department of Applied Physics

15. Aberration Monochromatic Aberrations: Maclaurin’s expansion: The Gaussian theory is the first order theory. For larger inclination angles, third order theory has to be used. Departures from the first order theory are known as monochromatic aberrations. Spherical Aberrations: (a) Longitudinal and transverse spherical aberrations. Fp´ and Fm´ are the focal points of the paraxial and marginal rays respectively. (b) Graphical representation of the longitudinal spherical aberration. Optics 1----by Dr.H.Huang, Department of Applied Physics

16. Aberration Minimize Spherical Aberrations The spherical aberration is reduced when the convex surface faces the distant object. In general, spherical aberration will be minimized when the refraction is equally shared between the surfaces. Optics 1----by Dr.H.Huang, Department of Applied Physics

17. Aberration Coma: Coma occurs with light from an off-axis object point and produces a comet-like spread of light in the image plane. Off-axis spherical aberration Tangential coma and Sagittal coma satisfies: Abbe’s sine condition is used for the elimination of coma Optics 1----by Dr.H.Huang, Department of Applied Physics

18. Aberration Oblique Astigmatism: Oblique astigmatism arises from the fact that the fans of rays in the two meridian DE and AC have different angles of incidence at the lens, giving rise to different foci along the direction of propagation. Optics 1----by Dr.H.Huang, Department of Applied Physics

19. Aberration Oblique Astigmatism: The relative position of the image points formed from axis and off-axis object points. The distance TTTS between the two focal lines in the astigmatic pencil is referred to as the astigmatic difference in the image. The difference between the emergent vergences in the tangential and sagittal meridians is called the astigmatic error for the particular obliquity of the incident light. Optics 1----by Dr.H.Huang, Department of Applied Physics

20. Aberration Oblique Astigmatism: T and S shells. The discs of least confusion lie on the shell marked D. The magnitude of the astigmatic difference TS depends on the form of the lens (known as bending). For object point at fairly small angular distance from the axis, astigmatism is less significant than coma, while the reverse is true at larger angles. Optics 1----by Dr.H.Huang, Department of Applied Physics

21. Aberration Petzval, Tangential and Sagittal Surfaces Curvature of Field: A planar object is imaged on a curved surface. Petzval curvature may be measured in terms of the distance p along the chief ray between the Petzval surface and the ideal image plane. The Petzval sum is, Optics 1----by Dr.H.Huang, Department of Applied Physics

22. Aberration Distortion: due to variation in lateral magnification A rear positioned stop introduces pincushion distortion. A front positioned stop introduces barrel distortion. Optics 1----by Dr.H.Huang, Department of Applied Physics

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