In bifocals, trifocals and progressive lenses from ZEISS the measured near power differs from the prescribed power for two reasons:
A trial lens (TL) displays a lower center thickness than a finished eyeglass lens (SL) with the same vertex power. As the diagram shows, the principal planes of the eyeglass lens are closer to the convex side of the lens than those of the trial lens. This results in different back focal lengths (f’TL < f’SL ), while the back vertex focal lengths are identical (f’v TL = f’v SL ). As the reciprocal of the focal length f’ equals the equivalent power F and the reciprocal of the back vertex focal length f’v equals the back vertex power F’v, the trial lens and the eyeglass lens have different equivalent powers F, but the same back vertex powers F’v.
If an object at a reading distance of 40 cm is sharply imaged through a trial lens with F’v = + 5.00 D , the same object is imaged by a eyeglass lens displaying the same dioptric power and with the same corneal vertex distance behind the retina. The lens power is too weak for the wearer.
To ensure that the finished eyeglass lens has the same reading power as the trial lens during refraction, the required correction value is added. The lens then has more positive back vertex power. In the above example, a lens with F’v = + 5.25 D would be required.
The dioptric power of a lens always depends on the ray path for which it was determined. In bifocal, trifocal and progressive lenses in particular, the ray path during use of the lenses for near vision differs considerably from the measuring ray path. It is for this reason that a different dioptric power is measured in the focimeter from that effective in front of the patient’s eye.
When using the lenses for near vision, however, a different ray path is present.
Here, a divergent ray bundle emerges from a near object. In near vision, prismatic effects in the near reference point of the lens cause a deviation of the central imaging principal ray, with the result that the principal ray is not perpendicular to the back surface of the lens. The dioptric power in front of the eye is not the same as that measured in the focimeter. ZEISS lenses are produced so that the prescribed power is actually present in front of the eye. The power measured in the focimeter is specified on the lens packet.
Due to the oblique ray bundle, additional astigmatic error occurs in near vision and must be corrected. This corrective value is also taken into account in all bifocal, trifocal and progressive lenses from ZEISS.
The measured near power of all ZEISS multifocal lenses is corrected as follows:
The Rx power for near vision is specified for a standardized situation of use. For additions to + 2.50 D, the measured powers of ZEISS lenses are calculated for a distance of 380 mm. For additions over 2.75 D, the working distance becomes smaller, making a calculation necessary for each addition (object distance [mm] = 1000/Add.).
The lens packets for bifocal, trifocal and progressive lenses from ZEISS specify both the prescribed power and the measured power.
The sole purpose of the specified measured power for near vision is to allow the lens to be checked in the focimeter. If the same value is measured with the focimeter as that given on the lens packet, the prescribed reading powers will be effective for the standardized situation of use when wearing.
The measured values are specified as the powers in the two principal meridians and as the axis of the first principal meridian.
|+ 4.00||+ 2.00||180||+ 3.00|
|Measured powers||1st principal meridian||2nd principal meridian||Axis|
|Distance||+ 4.00||+ 6.00||180|
|Near||+ 7.26||+ 9.40||1|
To determine the distance and reading powers of bifocal, trifocal and progressive lenses from ZEISS, the concave side of the lens should be placed on the focimeter support. The specified measured values can be checked directly in the major reference points for near and distance vision.
The measured value in the major reference point for distance vision is measured in the semicircle (distance measuring circle) above the distance centering cross.
The measured value for near vision can be checked in the lower measuring circle.
Measuring bifocals and trifocals
The dioptric power in the major reference points for distance and near vision are measured in the same way as for single vision lenses. The measured reading power is checked in the major reference point for near vision which is located 5 mm below the segment top in bifocal lenses.
A distinction is also made between measured and Rx powers in prismatic lenses from ZEISS. One reason for this is the different geometry of prismatic trial lenses and prismatic eyeglass lenses. Another is the different ray paths present during measurement in the focimeter and when wearing.
In prismatic prescriptions, the prism should not be generated by decentration under any circumstances as this results in considerably poorer visual quality than that obtained with lenses ordered with prism.