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Retinoscopy
Loknath Goswami
B.Sc Optom 2nd year
Ridley College of Optometry
Jorhat, Assam
Introduction
• Retinoscopy is an objective method of
measuring the optical power of the eye
• It is used to illuminate the inside of the eye
and to observe the light that is reflected from
the retina
• These reflected rays change as they pass out
through the optical components of the eye,
and by examining just how these emerging
rays change, we determine the refractive
power of the eye
Evolution of retinoscopy
• 1859 – Sir William Bowman commented on
the peculiar linear fundus reflex he saw when
viewing astigmatic eyes with Helmholtz’s new
ophthalmoscope
• 1873 – The first objective diagnosis of
refractive errors was by the french
ophthalmologist Cuignet (Father of
Retinoscopy)
• 1878 – Mengin published the clear and simple
explanation that helped to popularize the
retinoscopic technique
• 1880 – Parent, published his explanation of
quantified objective refraction
• 1903 – Duane first advocated the systematic
use of cylindrical lenses for retinoscopy in
astigmatism
Copeland’s contributions
Around 1920, Jack C. Copeland was using
one of Wolff’s original European spot
retinscopes, when he dropped the instrument on
the floor, damaging the bulb filament. When
reexamining the schematic eye that he was
working with, he noted a difference in the
reflexes, and set about solving what had
happened. From this original observation came
the streak retinoscopic technique that is taught
today
• 1927 – Copeland patented his original model,
popularized the streak technique and
revolutionized retinoscopy
• The instrument has five flaws that Copeland
corrected in his improved version, marketed
since 1968 as Optec 360
Advantages
 Reduces the refraction time and error
 Minimizes decisions that the patient has to
make
 Extremely important when communication is
difficult or impossible
- Retarded, deaf persons
- Foreigners
- Children, infants
• By evaluating the retinoscopic reflex, we can
also detect aberrations of the cornea and of
the lens, as well as opacities of the ocular
media
Types
• Reflecting mirror retinoscope
– Plane mirror retinoscope
– Priestly-Smith’s mirror retinoscope
• Self illuminated retinoscope
– Spot retinoscope
– Streak retinoscope
Plane mirror retinoscope
Reflecting mirror retinoscope
• A perforated mirror by which the beam is
reflected into the patient’s eye and through a
central hole the emergent rays enter the
observer’s eye
• Movements of the illuminated retinal areas
are produced by tilting a mirror, either a
plane or concave
Reflecting mirror retinoscope
Advantages
• Cheaper than the self
illuminated
Disadvantages
• Requires a separate light
source
• Glare from that source of
light is annoying to the
patient
• To check the axis and
amount of cylinder is
difficult
• Intensity and type of beam
cannot be changed or
controlled
Self illuminated retinoscope
• The light source and the mirror are
incorporated in one
• Streak – light source is a linear (uncoiled)
filament
• Spot – light source is projected round
The streak retinoscope
• The modern retinoscope differs from the
simple instrument previously described in two
respects
– It incorporates a concave mirror in addition to the
plane mirror
– The light source is in the form of a streak rather
than a spot
Parts of retinoscope head
Projection system
• Light source
• Condensing lens
• Mirror
• Focusing sleeve
• Current source
Projection system
The projection system is simple; the
retinoscope emits rays of light that illuminate
the retina (the pigment epithelium and choroid).
By turning the sleeve one can rotate the
projected streak, and by raising or lowering the
sleeve one can make the rays divergent or
convergent
Observation system
• Peep hole
• Mirror
– The mirror have an optical aperture; the central
slivering of the mirror is absent. Some models use
a semi-silvered (beam splitter) surface to
accomplish the same purpose
Handling the retinoscope
Hold the retinoscope in the right hand
before the right eye, and in the left hand when
using the left eye. Keeping both eyes open and
the lights low, hold the retinoscope against brow
and wiggle head or trunk perpendicular to the
streak axis
Motions
• Myopia – against motion is observed
• Hyperopia – with motion is observed
• Emmetropia – no motion known as neutral
motion or complete flashing
Reflex :With movement
Reflex :Against movement
Neutralized
Preliminary steps
• Set the sleeve in its lowest position (plano-
mirror effect)
• Position yourself 2/3 meter (26”) from the
patient. This distance implies a working lens of
+1.50D. The distance can be made to vary.
• With the refracting equipment in place, direct
the patient’s attention to a fixation spot at 15
feet or more from the eye and align the streak
vertically
• Observe the “reflex” which will appear
providing no oblique astigmatism is present
• If oblique astigmatism is present, the reflex
does not appear vertical
• Move the vertical streak horizontally across
the pupil and back again and observe whether
the reflex moves in the same direction as the
streak or in the opposite direction
• Rotate the control sleeve until the streak is
horizontal and move the streak vertically
• If the streak and the reflex move in the same
direction with no lens in the refractive
apparatus, refraction is one of these:
– Hyperopia
– Emmetropia
– Myopia of less than 1.50 diopters
If the reflex moves in the opposite direction, the error
is myopia greater than 1.50 dipoters
Determining refractive error by
neutralization
• Before starting, make sure the eye not being
refracted has some “against” motion using the
plano mirror effect. This will blur vision to
prevent accommodation
• If “with” or neutral motion is noticed initially,
place about a +1.00 sphere before the eye
once neutral motion is seen
Neutralising with spheres only
• Change sphere in the minus direction until the
reflexes in all axes have “with” motion
• Adjust in the plus direction until the reflex fills
the pupil in one meridian and all motion is
stopped. This will be one of the principal
meridians if astigmatism is present. That
meridian is then said to be neutralized
• Repeat the neutralization in the meridian 90˚
away
Confirmation of neutralization
1. Move the sleeve all the way up (concave
mirror position); the reflex should also
appear neutralized
2. Move closer to the patient and “with”
motion should return; move away and
“against” motion should appear
3. Place an extra +0.25 sphere in the apparatus
and “against” motion should appear
Locating the axis of astigmatism
• Two phenomena help in determining the axis of
astigmatism:
–Break
–Width
Break is observed when the streak is not
aligned with a principal meridian astigmatism.
The streak will be aligned with a principal
meridian when the break effect disappears and
the width of the reflex is narrowest ( and it
appears its brightest). Then continue with
neutralization as before
Interpretation of results
Hyperopia
• Hyperopia exists when, at the 2/3 meter
distance using the plano mirror effect, “with”
motion is neutralized using a plus lens greater
than +1.50 diopters and both meridians
neutralize with the same strength lens
• Total hyperopia is estimated by subtracting
1.50 diopters from the total strength lens
used. For example, if it takes a +2.50 lens to
neutralize motion at 2/3 meter, the total
hyperopic error is +1.00 diopter
Myopia
• When “with” motion, using the plano mirror
effect at 2/3 meter, is neutralized with a plus
lens of less than 1.50 D
• When at 2/3 meter, using the plano mirror
effect, no motion appears at all. The myopia is
then exactly 1.50 D
• When the motion is “against” using the plano
mirror effect, and is neutralized with a minus
lens
Astigmatism
• Astigmatism exists when the two principal
meridians neutralize with different strength
lenses. It may be present in many forms:
– Simple hyperopic
– Simple myopic
– Compound hyperopic
– Compound myopic
– In the mixed form
Astigmatism measurement
• Neutralize one principal meridian first. Then
add the appropriate plus or minus cylindrical
lens until the other principal meridian is
neutralized
• Neutralization may also be done by continuing
to add spherical lenses until the second
principal meridian is neutralized. Then the
astigmatic error is equal to the difference in
strength of lenses necessary to neutralize the
two meridians
Axis of astigmatism
• If the correcting cylinder is of the proper
power, a 10˚ error in axis will produce a new
astigmatism of approximately one third of the
strength of the original astigmatism with its
principal meridian at approximately 45˚ to
those of the original astigmatism
• The technique for setting the axis is reffered to
as “straddling”
Determination of axis
• When one have an approximate correction of
the refractive error and wish to refine the axis
setting, the following technique will be
helpful.
– Move up closer to the eye so that the edges of the
reflex can be seen
– Compare the widths of the two reflexes as you
rotate the streak 45˚ to either side of the
correcting cylinder axis
– Recede slowly while doing this. Compare the
widths of the two reflexes
– If there is an axis error, the reflex will be of
different widths in the two positions
– When using plus cylinders, one have to rotate the
axis toward the narrow band until the reflex
widths are equal
– When using minus cylinders, one have to rotate
the axis away from the narrow band
– When the reflex widths are equal, the proper axis
has been determined
References
• John M. Comboy, The retinoscopy book: an
introductory manual for eye care professionals
5th edition, pg no. 1 to 15
“ You can’t learn retinoscopy by reading a book. . .”
Jack C. Copeland
Retinoscope and retinoscopy

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Retinoscope and retinoscopy

  • 1. Retinoscopy Loknath Goswami B.Sc Optom 2nd year Ridley College of Optometry Jorhat, Assam
  • 2. Introduction • Retinoscopy is an objective method of measuring the optical power of the eye • It is used to illuminate the inside of the eye and to observe the light that is reflected from the retina • These reflected rays change as they pass out through the optical components of the eye, and by examining just how these emerging rays change, we determine the refractive power of the eye
  • 3. Evolution of retinoscopy • 1859 – Sir William Bowman commented on the peculiar linear fundus reflex he saw when viewing astigmatic eyes with Helmholtz’s new ophthalmoscope • 1873 – The first objective diagnosis of refractive errors was by the french ophthalmologist Cuignet (Father of Retinoscopy)
  • 4. • 1878 – Mengin published the clear and simple explanation that helped to popularize the retinoscopic technique • 1880 – Parent, published his explanation of quantified objective refraction • 1903 – Duane first advocated the systematic use of cylindrical lenses for retinoscopy in astigmatism
  • 5. Copeland’s contributions Around 1920, Jack C. Copeland was using one of Wolff’s original European spot retinscopes, when he dropped the instrument on the floor, damaging the bulb filament. When reexamining the schematic eye that he was working with, he noted a difference in the reflexes, and set about solving what had happened. From this original observation came the streak retinoscopic technique that is taught today
  • 6. • 1927 – Copeland patented his original model, popularized the streak technique and revolutionized retinoscopy • The instrument has five flaws that Copeland corrected in his improved version, marketed since 1968 as Optec 360
  • 7. Advantages  Reduces the refraction time and error  Minimizes decisions that the patient has to make  Extremely important when communication is difficult or impossible - Retarded, deaf persons - Foreigners - Children, infants
  • 8. • By evaluating the retinoscopic reflex, we can also detect aberrations of the cornea and of the lens, as well as opacities of the ocular media
  • 9. Types • Reflecting mirror retinoscope – Plane mirror retinoscope – Priestly-Smith’s mirror retinoscope • Self illuminated retinoscope – Spot retinoscope – Streak retinoscope
  • 11. Reflecting mirror retinoscope • A perforated mirror by which the beam is reflected into the patient’s eye and through a central hole the emergent rays enter the observer’s eye • Movements of the illuminated retinal areas are produced by tilting a mirror, either a plane or concave
  • 12. Reflecting mirror retinoscope Advantages • Cheaper than the self illuminated Disadvantages • Requires a separate light source • Glare from that source of light is annoying to the patient • To check the axis and amount of cylinder is difficult • Intensity and type of beam cannot be changed or controlled
  • 13. Self illuminated retinoscope • The light source and the mirror are incorporated in one • Streak – light source is a linear (uncoiled) filament • Spot – light source is projected round
  • 14. The streak retinoscope • The modern retinoscope differs from the simple instrument previously described in two respects – It incorporates a concave mirror in addition to the plane mirror – The light source is in the form of a streak rather than a spot
  • 16. Projection system • Light source • Condensing lens • Mirror • Focusing sleeve • Current source
  • 17. Projection system The projection system is simple; the retinoscope emits rays of light that illuminate the retina (the pigment epithelium and choroid). By turning the sleeve one can rotate the projected streak, and by raising or lowering the sleeve one can make the rays divergent or convergent
  • 18. Observation system • Peep hole • Mirror – The mirror have an optical aperture; the central slivering of the mirror is absent. Some models use a semi-silvered (beam splitter) surface to accomplish the same purpose
  • 19. Handling the retinoscope Hold the retinoscope in the right hand before the right eye, and in the left hand when using the left eye. Keeping both eyes open and the lights low, hold the retinoscope against brow and wiggle head or trunk perpendicular to the streak axis
  • 20. Motions • Myopia – against motion is observed • Hyperopia – with motion is observed • Emmetropia – no motion known as neutral motion or complete flashing
  • 24. Preliminary steps • Set the sleeve in its lowest position (plano- mirror effect) • Position yourself 2/3 meter (26”) from the patient. This distance implies a working lens of +1.50D. The distance can be made to vary. • With the refracting equipment in place, direct the patient’s attention to a fixation spot at 15 feet or more from the eye and align the streak vertically
  • 25. • Observe the “reflex” which will appear providing no oblique astigmatism is present • If oblique astigmatism is present, the reflex does not appear vertical • Move the vertical streak horizontally across the pupil and back again and observe whether the reflex moves in the same direction as the streak or in the opposite direction
  • 26. • Rotate the control sleeve until the streak is horizontal and move the streak vertically • If the streak and the reflex move in the same direction with no lens in the refractive apparatus, refraction is one of these: – Hyperopia – Emmetropia – Myopia of less than 1.50 diopters If the reflex moves in the opposite direction, the error is myopia greater than 1.50 dipoters
  • 27. Determining refractive error by neutralization • Before starting, make sure the eye not being refracted has some “against” motion using the plano mirror effect. This will blur vision to prevent accommodation • If “with” or neutral motion is noticed initially, place about a +1.00 sphere before the eye once neutral motion is seen
  • 28. Neutralising with spheres only • Change sphere in the minus direction until the reflexes in all axes have “with” motion • Adjust in the plus direction until the reflex fills the pupil in one meridian and all motion is stopped. This will be one of the principal meridians if astigmatism is present. That meridian is then said to be neutralized • Repeat the neutralization in the meridian 90˚ away
  • 29. Confirmation of neutralization 1. Move the sleeve all the way up (concave mirror position); the reflex should also appear neutralized 2. Move closer to the patient and “with” motion should return; move away and “against” motion should appear 3. Place an extra +0.25 sphere in the apparatus and “against” motion should appear
  • 30. Locating the axis of astigmatism • Two phenomena help in determining the axis of astigmatism: –Break –Width Break is observed when the streak is not aligned with a principal meridian astigmatism. The streak will be aligned with a principal meridian when the break effect disappears and the width of the reflex is narrowest ( and it appears its brightest). Then continue with neutralization as before
  • 32. Hyperopia • Hyperopia exists when, at the 2/3 meter distance using the plano mirror effect, “with” motion is neutralized using a plus lens greater than +1.50 diopters and both meridians neutralize with the same strength lens • Total hyperopia is estimated by subtracting 1.50 diopters from the total strength lens used. For example, if it takes a +2.50 lens to neutralize motion at 2/3 meter, the total hyperopic error is +1.00 diopter
  • 33. Myopia • When “with” motion, using the plano mirror effect at 2/3 meter, is neutralized with a plus lens of less than 1.50 D • When at 2/3 meter, using the plano mirror effect, no motion appears at all. The myopia is then exactly 1.50 D • When the motion is “against” using the plano mirror effect, and is neutralized with a minus lens
  • 34. Astigmatism • Astigmatism exists when the two principal meridians neutralize with different strength lenses. It may be present in many forms: – Simple hyperopic – Simple myopic – Compound hyperopic – Compound myopic – In the mixed form
  • 35. Astigmatism measurement • Neutralize one principal meridian first. Then add the appropriate plus or minus cylindrical lens until the other principal meridian is neutralized • Neutralization may also be done by continuing to add spherical lenses until the second principal meridian is neutralized. Then the astigmatic error is equal to the difference in strength of lenses necessary to neutralize the two meridians
  • 36. Axis of astigmatism • If the correcting cylinder is of the proper power, a 10˚ error in axis will produce a new astigmatism of approximately one third of the strength of the original astigmatism with its principal meridian at approximately 45˚ to those of the original astigmatism • The technique for setting the axis is reffered to as “straddling”
  • 37. Determination of axis • When one have an approximate correction of the refractive error and wish to refine the axis setting, the following technique will be helpful. – Move up closer to the eye so that the edges of the reflex can be seen – Compare the widths of the two reflexes as you rotate the streak 45˚ to either side of the correcting cylinder axis
  • 38. – Recede slowly while doing this. Compare the widths of the two reflexes – If there is an axis error, the reflex will be of different widths in the two positions – When using plus cylinders, one have to rotate the axis toward the narrow band until the reflex widths are equal – When using minus cylinders, one have to rotate the axis away from the narrow band – When the reflex widths are equal, the proper axis has been determined
  • 39. References • John M. Comboy, The retinoscopy book: an introductory manual for eye care professionals 5th edition, pg no. 1 to 15
  • 40. “ You can’t learn retinoscopy by reading a book. . .” Jack C. Copeland