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Learning from Giants’ Mistakes in Cataract Surgery
Fedorov 67 vs Fyodorov 75
Samir I Sayegh, MD, PhD, FACS, FAAO, FASRS
The EYE Center, Champaign, IL, USA
sayegh@umich.edu
Abstract
One of the most influential papers in the history of cataract surgery is Fedorov and Kolinko’s
1967 paper. All so called third and fourth generation intraocular lens calculation formulas
implemented to this day are based on it. We show that the actual expression given in the 1967
article is incorrect and was subsequently corrected by Fedorov and colleagues in 1975. We
show the source of error and comment on implications for modern day intraocular power
calculations for cataract surgery.
Introduction
Slava Fedorov’s contributions to Ophthalmology are profound and lasting. In a paper with
Albina Kolinko in 1967 they attempted a rational theoretical approach to the computation of
intraocular lens (IOL) power based on biometry of the patient’s eye1. The paper was written in
Russian and was followed by a few similar attempts by mainly European ophthalmologists. In
1975, together with Galin and Linksz, Fedorov (Fyodorov) contributed a similar article and
computation to the English literature2. This made the approach more accessible to a wider
readership and was followed by the (re)introduction of regression methods exemplified by
SRK3,4 and somewhat later, by a realization that theoretical methods were foundational and
need be adopted albeit with a grain of tweaking! This is represented by some of the major
“third generation” or “vergence based” formulas such as Holladay1, SRKT and HofferQ5,6,7, all of
which cite at least one of the Fyodorov and colleague’s papers and are in turn some of the most
cited and implemented papers in the IOL power calculation literature.
To our knowledge, there is no systematic comparison that has been attempted between the
1967 and 1975 versions of Fedorov and colleagues’ articles. In fact, a number of papers have
cited both the 1967 and 1975 articles without mention of any discrepancy4,6,8. Others will cite
only one9 or the other3,10,11. Some will mention a date and cite the article from the other
date12. Yet others, surprisingly, cite neither13. In the present work we start by a direct
comparison of the key formulas and their differences including numeric estimates and clinical
implications. We follow with an analysis of the original sources and the sources of errors and
draw conclusions as to lessons to be learned.
The 1967 and 1975 formulas of Fedorov and colleagues are different. One is incorrect.
1967 version1
!"#$ %&'( !
r)
* ( + ,&+
'&
-
.
* ( +
/0
&1(&+!
r
'&
2.
345
/
1975 version2
!6%& ' ( 7!8
.
7( +
/)
1(&+!8
'&
-.
359
/
where the symbols used in the corresponding articles and in our presentation are given in
tables 1 and 2 where ACD = Anterior Chamber Depth and ELP = Effective Lens Position.
Power
F67
F75
Sayegh
Cornea power
!r
!8
K
IOL power
!"#$
!:
L
EYE Power
!;<=
-
E
Table 1 Notations for Powers
Linear Measure
F67
F75
Sayegh
Sayegh-
Reduced
Axial length
*
a
a
>
Focal length
?@
-
f
A
Postoperative ACD (“ELP”)
k
k
e
B
Second principal plane to IOL
C@
-
*
D
Table 2 Notations for Distances and Reduced Distances
Our notation eliminates the use of subscripts, and while using familiar eye-specific symbols,
improves readability and makes explicit use of reduced distances. Powers are denoted by
capital Latin letters usually related to the corresponding refracting surface designation.
Distances are denoted by lower case Latin letters and the corresponding reduced distances
(distance/index of refraction) by the corresponding Greek letter.
The F67 – F75 difference and some numerical comparisons
Using Sayegh’s notation, F67 can be written as
E %&1(
)
>( F,&F
'&
-
G
.
> ( F
/.
&1(&FG
/
And F75 would read in same notation
E %& 1( >G
.
>( F
/.
&1(&FG
/
& &
H
.3I/.JKLMLNLOPQRKSTU/
V
the difference D = F67-F75 can then be expressed as
W&% BG
)
'( 1
'
-
.
> ( F
/.
1(BG
/.
W
/
Numerical examples are illustrated in Figure 1 where
W
is plotted as a function of the
postoperative ACD or ELP. For example, using a 3.2 mm anterior chamber depth, the average
reported by the authors, and for average values of keratometry and axial length, one finds a D
just short of 2 D between F67 and F75 with F67 ~ F75 + 2 D. Given that the F75 is the correct
derivation it is interesting to notice that the 67 paper comments that it is best to leave the
patients with 1-2 D of myopia as they will have no accommodation left1. Note that D is a strictly
increasing function of ELP and nearly doubles for an IOL placed in the bag of a “typical” eye.
Figure 1 The difference in diopters between the IOL power prediction of Fedorov 1967 and Fyodorov 1975
1967 Fedorov and Kolinko approach and error. Sources and sources of error.
F67 relies on and cites findings from the 1950 edition of a Russian language physiological optics
work by Kravkov (Кравков)14. The relations used are identical to those in Gullstrand 1909 and
191115. The approach of Fedorov 1967 boils down to the following: Treat the pseudophakic eye
as a “thick lens” with the first refractive surface being the cornea and the second the IOL.
Express the power of that eye in two ways. One as the combination of the power of the cornea
and that of the IOL, with the “thickness” being the postoperative ACD. The other as being the
inverse of the focal length (i.e. the reduced second principal plane distance from the retina),
which is expressed in terms of quantities including the axial length. Equating these two forms
for the power of the eye yields the expression of the IOL power in terms of axial length,
postoperative ACD, corneal power, and index of refraction of the aqueous/vitreous.
In more detail, what is done is the following.
1) Use the thick lens equation with the cornea and IOL as the two powers being combined
and the (postoperative) anterior chamber depth as the “thickness” of the combination
thick lens. The thick lens relation is referenced to Kravkov book p. 38. This approach
results in an expression for the power of the eye as a function of the powers of cornea
and IOL, the anterior chamber depth, and the index of refraction.
Referring to tables 1 and 2 and the description above, we have 3 powers and 4 reduced
lengths for a total of 7 variables. We can now write, in our compact notation, the two
equations involving the power of the eye:
X % G , E ( &F&G&E
0
.1/
(YZ[\+&*]'^&]_`7Y[a'
2
And:
X % 1
A&
.
b
/
(
.
?a\7*&*]'cYZ ( dae]f&f]*7Y[a'
/
2) Draw a diagram with 4 surfaces, A, B, C, D with A being the cornea plane and D the
retina plane with C being the IOL plane and B the second principal plane of the eye
(Figure 2).
Figure 2 Ada pted from Fedorov 67 with typos corr ected in green
Simple geometry shows
&&&&&&&&&&&&&&&&&g! %h!(hi ,gi
Or,
&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&?@% * ( + ,&C@
Where l is the axial length and k is the anterior chamber depth. In our compact notation:
? % 7 ( ], *
Or, equivalently, after division by the index of refraction
'
:
A % > ( F , D
.
j
/
3) In Fedorov 1967 article
?@
and
C@
are then expressed in terms of relationships known to
relate the powers and distances to the principal planes’ distances. Kravkov’s book14 has
a discussion of this based partially on Gullstrand’s contribution in von Helmholz’ third
edition of Physiological Optics (1909) and his 1911 monograph15. The main error in
Fedorov’s paper is introduced at this stage and the error is misinterpretation of a
formula in Kravkov and using a length instead of a reduced length (Figure 3). It is worth
noting that this 1967 paper by Fedorov is not cited in Fedorov 19752.
Finally, we express
D
in terms of the fraction of
F
:
D %&G
X&F
.
k
/
With four equations (1-4) we can, out of the 7 variables, eliminate 3, namely, E,
AlD
, leaving us
with one relation between the 4 remaining variables, L, K,
>
and
F
and we can thus express L in
terms of the other 3 variables as follows:
E %& 1
> ( F1(>G
1(FG
.
3I
/
This is trivially equivalent to F75 but not to F67. In Figure 3 we illustrate the error and the
correction that leads to results equivalent to F75.
Figure 3 Ada pted from Fedorov 67 with typos corrected in green and errors in red
The thick lens equation in its modern form can be attributed to Gauss16. More recent
treatments (prior to and following the Fedorov publications) can be easily found in the Optics
literature, from monumental foundational work17,18 to very useful practical manuals19. Prior to
the 1967 article, reviews of the classic Born and Wolf Optics text were already appearing
including in the biology literature.20
Discussion
Fedorov and Kolinko’
^
foundational equation as formulated in 1967 is a simple yet profoundly
insightful and influential approach to the calculation of the power of IOLs, yet it is incorrect. It
has been praised and cited for decades by generations of leading ophthalmologists that
proceeded to build on their legacy. The apparent lack of awareness or mention of the
differences between the 1967 version and the 1975 is stunning! This may be due to the fact
that the article was in Russian and published in the Russian literature. This is only partially
reasonable since there was a significant interest in “monitoring” Russian publications at the
height of the Cold War21 and even decades earlier keen interest in the scientific Russian
literature had already developed22. It is also worth mentioning that even current Russian
Ophthalmology literature continues to refer to that paper as foundational23.
Dogmatic views have sometimes persisted in Ophthalmology and in Medicine. Fairly recent
examples from cataract surgery include the A “constant” that has “no units” (AAO Basic and
Clinical Sciences, Lens and Cataract, various earlier editions, and persistent in recent quotes 24
despite clarifications 25) and the “constant” 30 degrees rotation for total loss of astigmatism
corrected by a toric IOL, and shown to be variable, implicitly by Felipe et al26 and explicitly by
Sayegh27. Various beliefs, rather than rigorous insight, continue to pervade the medical and
ophthalmological communities including a rising belief that artificial intelligence methods are all
powerful and can be a substitute for rigorously established scientific methodologies. It is
imperative to debunk such naïve beliefs and make sure that the rising generation of
ophthalmologists and vision scientists are schooled in the most rigorous intellectual tradition.
It is undeniable that the work by Fedorov and Kolinko constitutes one of the pillars of a
paradigm shift that, along with high quality intraocular lenses delivered through smaller
incisions and a number of other innovations, moved cataract surgery from a risk prone
procedure with moderate outcomes to one of the most sophisticated and successful
procedures in the history of Medicine12,28. This shift took place mainly in the last quarter of the
20th century and is ongoing. To continue building on this success it behooves us to reach a full
assimilation of the process it took to get where we are and delve into the methods and their
derivations. Maintaining a healthy centuries-old intellectual and scientific tradition is also likely
to accelerate our future progress towards better results for our patients.
Fully understanding giants’ mistakes, while standing on their shoulders, is a most valuable
building block of our next glorious pyramid!
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