The Essence of Spectacle Correction

The Essence of Spectacle Correction

The Essence of Spectacle Correction Basic Optics, Chapter 6 2 Spectacle/CL Correction The Hyperopic Eye A and B are conjugate points Far Point “ B “ A Last chapter, we saw that refractive error is in essence a Far Point problem. Recall that the far point is the location in optical space that is conjugate with the retina when the eye is not accommodating, and is therefore the optical location that is in sharp focus in the unaccommodated state. The emmetropic eye has its far point at infinity; thus, emmetropes see 20/20 at distance without correction. In contrast, the myopic eye has its far point (and hence clear vision) just anterior to the cornea, whereas the hyperopic eye’s far point is behind the globe. How are we going to provide myopes and hyperopes with clear vision at distance? Consider the myopic eye first. The Myopic Eye A and B are conjugate points “ B “ Far Point A Distance << Infinity (<20 feet) 3 Spectacle/CL Correction The Myopic Eye Parallel rays from infinity (vergence = 0) Far Point of the eye The goal of refractive correction is to provide clear vision at infinity. But a myopic eye is in focus only at its far point, just anterior to the corneal plane. Absent refractive surgery, there’s no changing or escaping this fact. 4 Spectacle/CL Correction The Myopic Eye Parallel rays from infinity (vergence = 0) Far Point of the eye Secondary Focal Point of the corrective lens The goal of refractive correction is to provide clear vision at infinity. But a myopic eye is in focus only at its far point, just anterior to the corneal plane. Absent refractive surgery, there’s no changing or escaping this fact. Spectacle/CL correction exploits the far point to provide clear distance vision. A lens is placed in front of the eye such that its secondary focal point coincides with the far point of the eye. 5 Spectacle/CL Correction The Myopic Eye Parallel rays from infinity (vergence = 0) Far Point of the eye Secondary Focal Point of the corrective lens The goal of refractive correction is to provide clear vision at infinity. But a myopic eye is in focus only at its far point, just anterior to the corneal plane. Absent refractive surgery, there’s no changing or escaping this fact. Spectacle/CL correction exploits the far point to provide clear distance vision. A lens is placed in front of the eye such that its secondary focal point coincides with the far point of the eye. As rays pass through the lens, they are refracted so that they form an image at the secondary focal point (remember, that’s the definition of the secondary focal point—it’s where parallel rays form an image). 6 Spectacle/CL Correction The Myopic Eye Parallel rays from infinity (vergence = 0) Far Point of the eye Secondary Focal Point of the corrective lens The goal of refractive correction is to provide clear vision at infinity. But a myopic eye is in focus only at its far point, just anterior to the corneal plane. Absent refractive surgery, there’s no changing or escaping this fact. Spectacle/CL correction exploits the far point to provide clear distance vision. A lens is placed in front of the eye such that its secondary focal point coincides with the far point of the eye. As rays pass through the lens, they are refracted so that they form an image at the secondary focal point (remember, that’s the definition of the secondary focal point—it’s where parallel rays form an image). Because the secondary focal point of the corrective lens coincides with the eye’s far point, the rays forming the image end up focused sharply on the retina. 7 Spectacle/CL Correction The Hyperopic Eye Far Point of the eye Parallel rays from infinity (vergence = 0) Secondary Focal Point of the corrective lens Spectacle/CL correction of hyperopia works the same way. A lens is selected that has its secondary focal point at the same location as the eye’s far point, posterior to the corneal plane. The resulting added convergence places parallel rays sharply on the retina. 8 Spectacle/CL Correction Parallel rays from infinity (vergence = 0) Far Point Secondary Focal Point So we could summarize refraction thusly: Place a lens in front of an eye so that the secondary focal point of the lens coincides with the far point of the eye. That’s all there is to it! Parallel rays from infinity (vergence = 0) Far Point Secondary Focal Point.

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