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Fundamentals of Progressive Lens Design - Laramy-K Optical

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Since each point in the blending region <strong>of</strong> a progressive<br />

lens can be thought <strong>of</strong> as a small cylinder, it makes sense<br />

to evaluate the optics <strong>of</strong> a progressive lens by measuring<br />

the amount <strong>of</strong> cylinder power present at these points.<br />

These measurements are <strong>of</strong>ten represented using a<br />

contour plot, which is a map that indicates how the levels <strong>of</strong><br />

an optical quantity vary across the lens (Figure 4).<br />

Astigmatism contour plots indicate regions <strong>of</strong> potential blur,<br />

image swim, and distortion, and are useful for predicting<br />

the size <strong>of</strong> the distance, intermediate, and near zones.<br />

Figure 4. Contour plots show the distribution <strong>of</strong> an optical<br />

quantity across the lens by indicating its levels in fixed<br />

intervals (e.g., 0.50 diopters).<br />

Generally speaking, progressive lenses have a unique<br />

astigmatism plot, so these plots serve as a kind <strong>of</strong><br />

“fingerprint” <strong>of</strong> the lens design. It is also useful to evaluate<br />

the distribution <strong>of</strong> Add power across the lens. Since most<br />

points across the surface contain cylinder, the spherical<br />

equivalent, or mean power, is measured, which is the<br />

average power <strong>of</strong> the lens surface at each <strong>of</strong> these points.<br />

Mean power contour plots indicate the location <strong>of</strong> the near<br />

zone, as well as regions <strong>of</strong> excess Plus power that may<br />

interfere with clear distance vision.<br />

While plots <strong>of</strong> surface astigmatism and mean Add power<br />

are the most common measures <strong>of</strong> optical performance,<br />

they fail to represent the combined interaction <strong>of</strong> these<br />

effects upon vision. Both unwanted cylinder power and<br />

excess—or insufficient—Add power contribute to blur. RMS<br />

(root-mean-square) power combines both the astigmatic<br />

and mean power errors into a single measure <strong>of</strong> power.<br />

RMS power is a more clinically meaningful measure <strong>of</strong><br />

optical performance, and a useful predictor <strong>of</strong> blur and<br />

visual acuity. 1<br />

Although less common, it is also possible to characterize<br />

the optics <strong>of</strong> a progressive lens using wavefront analysis.<br />

Wavefront analysis evaluates “higher order” aberrations,<br />

including spherical aberration and forms <strong>of</strong> coma, in<br />

addition to mean power and astigmatism—which are the<br />

“lower order” aberrations that are usually more detrimental<br />

to vision. Wavefront aberrations are <strong>of</strong>ten represented<br />

using either a Zernike series or a Taylor series, which are<br />

mathematical functions whose terms represent quantities<br />

such as mean power error, astigmatism, coma, and so on.<br />

Surface astigmatism and mean power contour plots provide<br />

a convenient way to represent various optical quantities,<br />

but they are only indicative <strong>of</strong> performance. Furthermore,<br />

contour plots <strong>of</strong> surface power are usually less visually<br />

meaningful than contour plots <strong>of</strong> ray-traced optical<br />

performance. These plots are calculated using lens-eye<br />

modeling to determine how the wearer actually perceives<br />

the optics <strong>of</strong> the lens.<br />

Minkwitz’s Theorem<br />

In well-designed progressive lenses, unwanted cylinder<br />

power in the periphery is generally reduced to its<br />

mathematical limits. However, some level <strong>of</strong> unwanted<br />

cylinder power is ultimately necessary in order to blend any<br />

surface with Add power. Minkwitz showed that the rate <strong>of</strong><br />

change in unwanted cylinder power (∆Cyl) at a small<br />

distance away from the centerline <strong>of</strong> the progressive<br />

corridor is nearly equal to twice the rate <strong>of</strong> change in Add<br />

power (∆Add) over an equal distance along the centerline<br />

<strong>of</strong> the corridor (Figure 5). 2<br />

Figure 5. Minkwitz’s theorem states that, in the vicinity <strong>of</strong> the<br />

progressive corridor, the cylinder power lateral to the corridor<br />

increases twice as fast as the Add power increases along the<br />

corridor—or ∆Cyl ≈ 2 × ∆Add.<br />

The average rate <strong>of</strong> change in Add power along the<br />

progressive corridor is equal to the total Add power divided<br />

by the corridor length <strong>of</strong> the lens (i.e., ∆Add = Add ÷<br />

Corridor). This means that the average rate <strong>of</strong> change in<br />

Add power is proportional to the Add power and inversely<br />

proportional to the corridor length <strong>of</strong> the lens design.<br />

Therefore, Minkwitz’s theorem demonstrates two important<br />

guidelines regarding the optics in the central regions <strong>of</strong> a<br />

progressive lens surface:<br />

1. The rate <strong>of</strong> change in cylinder power away from the<br />

progressive corridor increases as the length <strong>of</strong> the<br />

progressive corridor decreases. This means that lens<br />

designs with shorter corridors will produce more<br />

unwanted cylinder power or smaller viewing zones.<br />

2. The rate <strong>of</strong> change in cylinder power away from the<br />

progressive corridor increases as the Add power <strong>of</strong> the<br />

lens increases. This means the unwanted cylinder<br />

power in the periphery increases at roughly the same<br />

rate as the specified Add power (Figure 6).<br />

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