- •Contents
- •General Introduction
- •Objectives
- •1 Geometric Optics
- •Rays, Refraction, and Reflection
- •Introduction
- •Point Sources, Pencils, and Beams of Light
- •Object Characteristics
- •Image Characteristics
- •Magnification
- •Image Location
- •Depth of Focus
- •Image Quality
- •Light Propagation
- •Optical Media and Refractive Index
- •Law of Rectilinear Propagation
- •Optical Interfaces
- •Law of Reflection (Specular Reflection)
- •Law of Refraction (Specular Transmission)
- •Normal Incidence
- •Total Internal Reflection
- •Dispersion
- •Reflection and Refraction at Curved Surfaces
- •The Fermat Principle
- •Pinhole Imaging
- •Locating the Image: The Lensmaker’s Equation
- •Ophthalmic Lenses
- •Vergence
- •Reduced Vergence
- •Thin-Lens Approximation
- •Lens Combinations
- •Virtual Images and Objects
- •Focal Points and Planes
- •Paraxial Ray Tracing Through Convex Spherical Lenses
- •Paraxial Ray Tracing Through Concave Spherical Lenses
- •Objects and Images at Infinity
- •Principal Planes and Points
- •Section Exercises
- •Focal Lengths
- •Gaussian Reduction
- •Knapp’s Law, the Badal Principle, and the Lensmeter
- •Afocal Systems
- •Section Exercises
- •Questions
- •Power of a Lens in a Medium
- •Spherical Interface and Thick Lenses
- •Thick Lens
- •Back Vertex Power Is Not True Power
- •Aberrations of Ophthalmic Lenses
- •Third-Order Seidel Aberrations
- •Chromatic Aberrations
- •Avoiding Aberrations
- •Mirrors
- •Reflection From a Plane Mirror
- •Spherically Curved Mirrors
- •Reversal of the Image Space
- •The Central Ray for Mirrors
- •Vergence Calculations for Mirrors
- •Spherocylindrical Lenses
- •Combination of Spherocylindrical Lenses
- •The Conoid of Sturm
- •The Jackson Cross Cylinder
- •Prisms
- •Prism Diopter
- •Prismatic Effect of Lenses and the Prentice Rule
- •Prism Aberrations
- •Fresnel Prisms
- •Chapter Exercises
- •Questions
- •Appendix 1.1
- •Quick Review of Angles, Trigonometry, and the Pythagorean Theorem
- •Appendix 1.2
- •Light Properties and First-Order Optics
- •2 Optics of the Human Eye
- •The Human Eye as an Optical System
- •Schematic Eyes
- •Important Axes of the Eye
- •Pupil Size and Its Effect on Visual Resolution
- •Visual Acuity
- •Contrast Sensitivity and the Contrast Sensitivity Function
- •Refractive States of the Eyes
- •Binocular States of the Eyes
- •Accommodation and Presbyopia
- •Epidemiology of Refractive Errors
- •Developmental Myopia
- •Developmental Hyperopia
- •Prevention of Refractive Errors
- •Chapter Exercises
- •Questions
- •3 Clinical Refraction
- •Objective Refraction Technique: Retinoscopy
- •Positioning and Alignment
- •Fixation and Fogging
- •The Retinal Reflex
- •The Correcting Lens
- •Finding Neutrality
- •Retinoscopy of Regular Astigmatism
- •Aberrations of the Retinoscopic Reflex
- •Subjective Refraction Techniques
- •Astigmatic Dial Technique
- •Stenopeic Slit Technique
- •Cross-Cylinder Technique
- •Refining the Sphere
- •Binocular Balance
- •Cycloplegic and Noncycloplegic Refraction
- •Overrefraction
- •Spectacle Correction of Ametropias
- •Spherical Correcting Lenses and the Far Point Concept
- •The Importance of Vertex Distance
- •Cylindrical Correcting Lenses and the Far Point Concept
- •Prescribing for Children
- •Myopia
- •Hyperopia
- •Anisometropia
- •Clinical Accommodative Problems
- •Presbyopia
- •Accommodative Insufficiency
- •Accommodative Excess
- •Accommodative Convergence/Accommodation Ratio
- •Effect of Spectacle and Contact Lens Correction on Accommodation and Convergence
- •Prescribing Multifocal Lenses
- •Determining the Add Power of a Bifocal Lens
- •Types of Bifocal Lenses
- •Trifocal Lenses
- •Progressive Addition Lenses
- •The Prentice Rule and Bifocal Lens Design
- •Occupation and Bifocal Segment
- •Prescribing Special Lenses
- •Aphakic Lenses
- •Absorptive Lenses
- •Special Lens Materials
- •Therapeutic Use of Prisms
- •Chapter Exercises
- •Questions
- •Appendix 3.1
- •Common Guidelines for Prescribing Cylinders for Spectacle Correction
- •4 Contact Lenses
- •Introduction
- •Contact Lens Glossary
- •Clinically Important Features of Contact Lens Optics
- •Field of Vision
- •Image Size
- •Accommodation
- •Convergence Demands
- •Tear Lens
- •Correcting Astigmatism
- •Correcting Presbyopia
- •Contact Lens Materials and Manufacturing
- •Materials
- •Manufacturing
- •Patient Examination and Contact Lens Selection
- •Patient Examination
- •Contact Lens Selection
- •Contact Lens Fitting
- •Soft Contact Lenses
- •Rigid Gas-Permeable Contact Lenses
- •Toric Soft Contact Lenses
- •Contact Lenses for Presbyopia
- •Keratoconus and the Abnormal Cornea
- •Contact Lens Overrefraction
- •Gas-Permeable Scleral Contact Lenses
- •Therapeutic Lens Usage
- •Orthokeratology and Corneal Reshaping
- •Custom Contact Lenses and Wavefront Technology
- •Contact Lens Care and Solutions
- •Contact Lens–Related Problems and Complications
- •Infections
- •Hypoxic/Metabolic Problems
- •Toxicity
- •Mechanical Problems
- •Inflammation
- •Chapter Exercises
- •Questions
- •Appendix 4.1
- •Transmission of Human Immunodeficiency Virus in Contact Lens Care
- •Appendix 4.2
- •Federal Law and Contact Lenses
- •5 Intraocular Lenses
- •Intraocular Lens Designs
- •Classification
- •Background
- •Optical Considerations for Intraocular Lenses
- •Intraocular Lens Power Calculation
- •Piggyback and Supplemental Intraocular Lenses
- •Intraocular Lens Power Calculation After Corneal Refractive Surgery
- •Instrument Error
- •Index of Refraction Error
- •Formula Error
- •Power Calculation Methods for the Post–Keratorefractive Procedure Eye
- •Intraocular Lens Power in Corneal Transplant Eyes
- •Silicone Oil Eyes
- •Pediatric Eyes
- •Image Magnification
- •Lens-Related Vision Disturbances
- •Nonspherical Optics
- •Multifocal Intraocular Lenses
- •Types of Multifocal Intraocular Lenses
- •Clinical Results of Multifocal Intraocular Lenses
- •Accommodating Intraocular Lenses
- •Intraocular Lens Standards
- •Chapter Exercises
- •Questions
- •Appendix 5.1
- •History of Intraocular Lens Design
- •6 Optical Considerations in Keratorefractive Surgery
- •Corneal Shape
- •Angle Kappa
- •Pupil Size
- •Irregular Astigmatism
- •Application of Wavefront Analysis in Irregular Astigmatism
- •Causes of Irregular Astigmatism
- •Conclusion
- •Chapter Exercises
- •Questions
- •7 Optical Instruments and Low Vision Aids
- •Magnification
- •Telescopes
- •Galilean Telescope
- •Astronomical Telescope
- •Accommodation Through a Telescope
- •Surgical Loupe
- •General Principles of Optical Engineering
- •Terminology
- •Measurements of Performance of Optical Systems
- •Optical Instruments and Techniques Used in Ophthalmic Practice
- •Direct Ophthalmoscope
- •Indirect Ophthalmoscope
- •Fundus Camera
- •Slit-Lamp Biomicroscope
- •Gonioscopy
- •Surgical Microscope
- •Geneva Lens Clock
- •Lensmeter
- •Knapp’s Rule
- •Optical Pachymeter
- •Applanation Tonometry
- •Specular Microscopy
- •Keratometer
- •Topography
- •Ultrasonography of the Eye and Orbit
- •Macular Function Tests
- •Scanning Laser Ophthalmoscopes
- •Scheimpflug Camera
- •Autorefractors
- •Optical Coherence Tomography
- •Optical Aids
- •Magnifiers
- •Telescopes
- •Prisms
- •High-Add Spectacles
- •Nonoptical Aids
- •Electronic Devices
- •Lighting, Glare Control, and Contrast Enhancement
- •Nonvisual Assistance
- •Eccentric Viewing or Fixation Training
- •Instruction and Training
- •Chapter Exercises
- •Questions
- •Appendix 7.1
- •Approach to the Patient With Low Vision
- •8 Physical Optics
- •The Corpuscular Theory of Light
- •Diffraction
- •The Speed of Light
- •The Superposition of Waves
- •Coherence
- •Electromagnetic Waves
- •Polarization
- •Refractive Index and Dispersion
- •Reflection, Transmission, and Absorption
- •The Electromagnetic Spectrum
- •Frequency and Color
- •Energy in an Electromagnetic Wave
- •Quantum Theory
- •Light Sources
- •Thermal Sources
- •Luminescent Sources
- •Fluorescence
- •Phosphorescence
- •Lasers
- •Light–Tissue Interactions
- •Photocoagulation
- •Photoablation
- •Photodisruption
- •Photoactivation
- •Light Scattering
- •Rayleigh Scattering
- •Mie Scattering
- •The Tyndall Effect
- •Radiometry and Photometry
- •Light Hazards
- •Clinical Applications
- •Polarization
- •Interference
- •Diffraction
- •Imaging and the Point Spread Function
- •Image Quality—Modulation Transfer Function
- •Chapter Exercises
- •Questions
- •Appendix 8.1
- •Radiometric and Photometric Units
- •Basic Texts
- •Related Academy Materials
- •Requesting Continuing Medical Education Credit
Show Answer
8.6.Corneal haze secondary to corneal edema is primarily caused by
a.reflection
b.light scattering
c.refraction
d.diffraction
Show Answer
Appendix 8.1
Radiometric and Photometric Units
Understanding radiometry is a matter of not simply knowing the definitions of various units of measurement but also knowing how to use them appropriately. Every radiometric (or photometric) unit of measurement has a specific purpose.
In studying radiometry, it is helpful to think of light as a collection of photons. Broadband light consists of photons at many frequencies, whereas narrowband light consists of photons at just a few frequencies. For the purposes of this discussion, imagine it is possible to count every photon and identify its frequency.
Radiometry counts every photon—not just visible ones but also those at infrared and UV wavelengths, and all photons at wavelengths between 10 nm and 1 mm. Radiometric units are identified by the subscript (e). Spectral radiometry counts photons within a more limited range— whatever frequencies are of interest in a specific situation. Spectral radiometric units are identified by the subscript (λ).
Radiant energy (Qe)
Radiant energy (Qe) is the total energy produced, typically expressed in joules. Every photon produced by a source is counted, and its energy is calculated using E = hν. For example, an incandescent lightbulb produces not only visible light but also infrared and even some UV light, and photons from each of these spectra need to be included to determine the value for Qe. Also, Qe is a cumulative measurement; that is, it is taken over time. The Qe value for an incandescent bulb operating for 2 hours is twice that for the same bulb operating for 1 hour.
Qe (or Qλ) is the appropriate quantity when cumulative exposure is important. For instance, there is some evidence that cases of post–cataract-extraction cystoid macular edema are related to microscope illumination. Investigators should consider Qe (as well as other parameters) in evaluating light hazards.
Fluence (He)
Fluence (He) is a measure of energy density and is defined as radiant energy (Qe) divided by area.
For example, 6 J of radiant energy applied to an area of 2 cm2 equals a fluence of 3 J/cm2. Fluence measurements are often used clinically in association with laser ablation and photodynamic therapy (PDT).
Photoablation breaks chemical bonds, and in laser in situ keratomileusis (LASIK) or photorefractive keratectomy (PRK), the number of chemical bonds to be broken by a single laser pulse is proportional to the area of the laser beam. If the pulse energy is low in comparison with the beam area, too few bonds will be broken and the resulting ablation will be uneven. Similarly, in PDT the number of verteporfin molecules to be activated depends on the area of the lesion. Fluence is the appropriate radiometric unit to employ for calibrating lasers used for these procedures.
Radiant flux (Φe)
The word flux means flow, and radiant flux (Φe) is the amount of radiant energy emitted by a source or striking a surface per unit of time. It is a measure of power, typically expressed in joules per second, or watts. A source radiating 60 J for 1 minute produces a radiant flux of 1 W (60 J/60 s).
Irradiance (Ee) or exitance (Me)
Irradiance (Ee) is radiant energy divided by area and time, and it is typically expressed in watts per square meter or watts per square centimeter. For example, a 0.25 cm2 surface illuminated by 2 W has an irradiance of 2 W/0.25 cm2 = 8 W/cm2. Irradiance is used for surfaces illuminated by an external source, but the term radiant exitance (Me) may be used instead when the surface itself is the light source (eg, a light box used to view x-rays). However, irradiance and radiant exitance both have the same units (W/cm2), so some authorities use irradiance in both cases. Clinically, irradiance is the appropriate unit of measurement for photocoagulation equipment.
Radiant intensity (Ie)
Measurements of radiant intensity account for the directional properties of a light source. For example, a flashlight beam diverges somewhat but propagates in the same direction. Some flashlight beams are more narrowly divergent than others, whereas laser beams are extremely directional. It is therefore necessary to incorporate an angular measurement in the description of such light sources, a function served by radiant intensity (Ie), expressed as the radiant flux per unit solid angle or watts per steradian (W/sr).
Radiance (Le)
The measurement of radiance (Le) takes into account irradiance and radiant intensity, and it is the radiometric unit most closely related to brightness. Radiance is radiant flux per unit area per steradian (sr), typically expressed as W/m2 sr.
Photometry
Photometry measures the human visual system’s psychophysical response to light; it is essentially radiometry that takes into account the varying response of the eye to light of different wavelengths.
Based on data from measurements of people, weighting factors (presented as luminous efficacy curves) have been developed for each wavelength of the visible spectrum. There are luminous efficacy curves for photopic and scotopic conditions.
Photometry is a straightforward extension of radiometry—each photon and its frequency are counted. Each photon’s energy is calculated and multiplied by the luminous efficacy for its frequency. (To cite a trivial example of the difference between radiometry and photometry, a source that emits only UV light has radiometric intensity but no luminous intensity.) Photometric units are analogous to radiometric units and are indicated by the same symbols but subscripted with (v) (for visual) instead of (e). Table 8-1 compares radiometric units with analogous photometric units.
Table 8-1
There are many ways to measure photometric quantities. For clinical use, SI units are often not the most convenient. Table 8-2 lists alternative units commonly used to measure illuminance and luminance and their conversion factors. To develop a “feel” for photometric units, Table 8-3 lists photometric values associated with visual functions.
Table 8-2
Table 8-3
The troland (Td) is a unit that estimates retinal illuminance based on source luminance. A source with a luminance of 1 nit produces a retinal illuminance of 1 Td when viewed through a 1 mm2 pupil. If the pupil area is 10 mm2, then the retinal illuminance is 10 Td.
