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LOGO Dr Sneha Thapliyal
OBJECTIVE REFRACTION
CLINICAL REFRACTION
Determines and corrects refractive errors
Objective refraction Subjective refraction
Essential in:
Young children
Mental disability
Language difficulty
Deaf or mute
OBJECTIVE METHODS OF
REFRACTION
1. Retinoscopy
2. Autorefractometry
3. Photorefraction
4. Electrophysiological method of objective
refraction
RETINOSCOPY/SKIASCOPY
/SHADOW TEST
 Objective method of finding out the error of
refraction by means of retinoscope
utilizing the technique of NEUTRALIZATION
Far point concept
 The far point of eye is defined as the point in space that is
conjugate with the fovea when accomodation is relaxed.
 Emmetropia: Parallel rays focus on fovea.
 Retina conjugate with infinity.
 Far point is at infinity.
 Ammetropias: Parallel rays do not focus on retina.
 Ammetropic eyes require a correcting lens to make retina
conjugate with infinity, i.e., to move far point to infinity
 Hyperopia: Deficient refractive power.
 Parallel rays focus behind retina.
 Far point is beyond infinity.
 Plus lens converges rays on to retina and conjugate
fovea with infinity.
Far point concept
 Myopia: Excessive refractive power.
 Parallel rays focus in front of retina.
 Far point is between infinity and eye.
 Minus lens diverges rays on to the retina and conjugate
fovea with infinity.
 Aspherical ammetropias:
 This indicates different types of astigmatism.
 This type of errors have two far points.
 As a set of rays converge at one place and other at different
place due to cornea not having same radius of curvature in all
the meridians.
Principle of retinoscopy:
 To bring the far point of patient at the
nodal point of the observer at the
working distance
NEUTRALIZATION
1. No movement of red
reflex = NEUTRAL POINT
2. Reversal with
overcorrection by 0.25 D
3. On alternating the
working distance, slight
forward, ‘with’ movement
and an ‘against’
movement by slight
backward movement.
PREREQUISITES FOR
RETINOSCOPY
PREREQUISITES FOR
RETINOSCOPY
1. Dark room: 6 m long
2. A trial set:
 64 pairs of Spherical lenses(plus and minus)
0.12D
0.25-4.0D
4.0-6.0D
6.0-14D
14-20D
0.25
0.51D2D
20 pairs of Cylindrical lenses (plus and
minus)
0.25-2.00D
2.0-6.0D
10 Prisms:
½ to 6
8,10,12
0.250.5
 Accessories:
Plano lenses
Opaque discs
Pinhole
Stenopaeic discs
Maddox rods
Red and Green glasses
3. A trail frame
 Light weight
 Aluminium alloy- 30 g
 Adjustable- horizontally and vertically
 3 compartments: spherical, cylindrical, prisms
 Cylindrical compartment : smooth and accurate rotation
 Side pieces should be joint- tilted while testing for near vision
 Back lens in trial frames should occupy as nearly as possible the
position of spectacle lens i.e. around 12 mm in front of the cornea.
4. Phoropter or refractor
 Turn the dial – change the lens before
the aperture of the viewing system
5. Distance-vision chart
6. Near vision charts
7. Retinoscope:
Invented by Dr Jack Copeland
REFLECTING (MIRROR)
RETINOSCOPES
Priestley-Smith’s mirror
Plane mirror
SELF-ILLUMINATED
RETINOSCOPES
Spot self-illuminous
Streak retinoscope
HEAD
NECK
HANDLE
SLEEVE UP
PEEPHOLE
SLEEVE DOWN
STREAK RETINOSCOPE
HEAD
HANDLE
NECK
MIRROR
LENS
SLEEVE
PARASTOP
BULB
BATTERIES
bulb
Dark mirror
Reflecting
mirror
Sleeve
 Observing the optics of retinoscope we find two main
systems
- Projection system:
Light source
Condensing lens
Focusing sleeve
Current source
- Obsevation system:
Peep hole
RETINOSCOPE AND IT’S
PARTS:
The retinoscope:
how it works?
 PROJECTION SYSTEM:
illuminates the retina
 Light source: a bulb with
linear filament that projects
a line or streak of light
 Condensing lens: focuses
rays from bulb onto the
mirror
 Mirror : placed in the head
of instrument at 45 degree
angle, it bends the path of
light at right angles to the
axis of the handle
 Focusing sleeve controls
 Meridian:Turning the sleeve rotates the streak of light.
 Vergence:By varying the distance between the lens and
the bulb
 Bulb: Moved up-Plane mirror effect(Parallel rays)
Moved down-Concave mirror effect(converging
rays)
 Lens: Moved up-Concave mirror effect
Moved down-Plane mirror effect
 In Copelands instrument,
 moving the sleeve up or down moves the bulb.
 Sleeve up creates plane mirror effect & sleeve down
creates concave mirror effect
Copeland type- fixed lens with moving bulb
 In other Retinoscopes,
 the lens rather than the bulb moves on moving the
sleeve
 Sleeve up creates a concave mirror effect & sleeve
down creates plane mirror effect
Fixed bulb type, the lens moves
 OBSERVATON SYTEM:
 Allows to see the retinal reflex
 Light reflected by the illuminated retina enters the
retinoscope, passes through an aperture in the
mirror & out of the peephole at the rear end of the
head.
Optics in Retinoscopy
 Illumination stage: light is directed into the
subject’s eye to illuminate the retina
 Reflex stage: image of the illuminated retina
is formed at subject’s far point
 Observation stage: image of the far point is
located by moving the illumination across the
fundus and noting the behavior of the luminous
reflex seen by the observer in the subject’s pupil
Clinician
So
S1
S2
Patient
The light in the pupil is called the
“ret reflex”
The final goal
Observer Subject
Reflex disappears
Reflex moves down,
i.e. with direction
of movement of light
Mirror tilts further forwards
Mirror tilts forwards
S2
S2
Far point behind
observers pupil
Within pupil
Outside pupil
No S2
S1
Far point behind observers
pupil.
With movement of reflex,
gradual change from red reflex
to no reflex
With movement
Observer Subject
Far point in front of
observers pupil
Reflex disappears
Reflex moves up,
i.e. against direction
of movement of light
Mirror tilts forwards
Mirror tilts further forwards
S2
S2
Within pupil
Outside pupil
No S2
S1
Far point in front of observers pupil.
Against movement of reflex,
gradual change from red reflex to no
reflex
Against movement
Reflecting mirror:
 Perforated mirror
 Central hole: 2.5mm anteriorly
4 mm posteriorly
 By a plane mirror, rays are slightly divergent causing
less illumination
 Small hole corresponding to the central hole reduces
illumination in pupillary area by causing central dark
patch
 Sides of the small hole are blackened to prevent
annoying reflexes from entering the eye
 Slightly concave mirror with central opening of 4mm
and focal length greater than the distance between
observer and patient; 150 cm
LUMINOUS
RETINOSCOPE
 Streak retinoscope is the most popular
 Both light source and mirror are incorporated
 Intensity and type of beam can be controlled.
 Two main techniques of retinoscopy
are
Static Retinoscopy:
 It is the refractive state
determined when patient fixates an
object at a distance of 6 m with
accomodation relaxed.
Dynamic Retinoscopy:
 The refractive state is
determined while the subject fixates
an object at some closer distance,
usually at or near the plane of
retinoscope itself with
accommodation under action.
RETINOSCOPY
TECHNIQUES:
PROCEDURE OF
RETINOSCOPY
 Patient is made to sit at a
distance of 2/3rd of a meter
 Accomodation should be
relaxed
 Use right eye for patient’s right
eye and left eye for left
 Trial frame is fitted
 Direct the light from retinoscope
into patient’s pupil
 Move the retinoscope in
horizontally and observe the red
reflex.
 Suitable lens is placed
before the eyes to
neutralize the band when
the pupil will be filled with
uniform light
 Now move vertically, if still
pupil is filled with uniform
light, no astigmatism.
Examiner sits just enough to the side
to avoid blocking patient’s fixation
Characteristics of the moving
retinal reflex
Speed and brilliance
Low refractive High refractive
Bright Faint
Moves rapidly Moves slowly
2.Width of reflex
Narrow Wide
High degree of ametropia Low degree of ametropia
3. Presence of astigmatism
When the axis does not correspond with the movement of the mirror,
the shadow appears to swirl around.
Examiner should scope both vertical and
horizontal meridian.
We correct the astigmatism with cylindrical
lens.
Cylindrical lens may be plus or minus, but
have power in only one meridian, that
which is perpendicular to the axis of the
cylinder.
The axis meridian is flat and has no
power.
ASTIGMATISM
CYLINDRICAL AXIS
 Break in the alignment
between the reflex in the
pupil and the band
outside it when the streak
is off the axis
 Rotate the streak until the
break disappears
 Width of the streak
appears narrowest when
the streak aligns with the
true axis.
STRADDLING
 Confirmation of axis
 Retinoscope streak- 45
degree off axis in both
directions
 Correct axis- width of
streak equal in both
positions
 Axis not correct- width is
unequal
 Narrow reflex is guide
towards which cylinder’s
axis should be turned
PROBLEMS IN
RETINOSCOPY:
1. Red reflex may not be visible or maybe poor
 Small pupil
 Hazy media
 High degree of refractive error
 Overcome by causing mydriasis and/or use of
converging light with concave mirror retinoscope
2. Changing retinoscopic findings
 Abnormally active accomodation
 Overcome by fogging retinoscopy and cycloplegic
3. Spherical aberrations
 Dilated pupils
4. Conflicting shadows
 Irregular astigmatism
5. Triangular shadows
 Conical cornea
www.phacotube.com
Scissoring shadows
Astigmatism
Overcome by: undilated
pupil
Cycloplegics in retinoscopy
 When retinoscopy is performed after instilling
cycloplegic drugs it is termed as Wet Retinoscopy
1. Atropine 1% ointment
 Used in children < 7yrs age
 Dose:1% eye ointment 3times daily for 3days
 Effect lasts for 10-20days
 Deduction for cycloplegia with atropine is 1D
2. Homatropine 2% drops
 Used in hypermetropes between 7 to 35yrs
 Dose:1drop instilled every 10mins for 6times &
retinoscopy is performed after 1-2hrs
 Effect lasts for 48-72hrs
 Deduction for cycloplegia with homatropine is
0.5D
3. Cyclopentolate I% drops
 Used in persons between 7 to 35yrs
 Dose:1drop instilled every 10mins for 3 times &
retinoscopy is performed after 1- 1 1/2hrs
 Effect lasts for 6 to 18hrs
 Deduction for cycloplegia with Cyclopentolate is
0.75D
 Only mydriatic [ 10% phenylephrine] may is used in
elderly patients to enhance the pupillary reflex when the
pupil is narrow or media is slightly hazy
 Later it should be counteracted by use of miotic drug[ 2%
pilocarpine]
Clinician
S2
Patient
We now have neutral
We have also introduced
negative vergence due to
our working distance
(WD)
= 1/d (m)
Where d = distance in m,
measured between your
ret and patient’s eye
We have added lenses
To get the right prescription
we need to compensate
Rx = lens power – 1/d
So to get neutral, we needed:
lens power = Rx + 1/d
Working distance
compensation
Calculation
 For example, if neutrality
is achieved with a
+3.00DS lens and your
working distance is 50cm
 Rx = +3.00DS – (1/0.50)
 = +3.00 – 2.00
 =+1.00DS
Working distance lens
 Before you begin, add a
“working distance lens”
 A +ve lens to cancel out
the negative vergence
 As in eg., WD = 50cm
 WD lens = 1/0.50 =
+2.00DS
 Neutrality for the same
patient is still +3.00DS
 WD lens = +2.00DS
 Lens power = +1.00DS
Rx = lens power - 1/d
AUTOREFRACTOMETRY
Alternative method of assessing error of
refraction by use of an optical equipment
called refractometer or optometer
OBJECTIVE SUBJECTIVE
History
 Collins(1937) developed the first semi automated electronic
refractionometer.
 Safir (1964) automated the retinoscope and this work led to
the first commercial autorefractor-the Ophthalmometron.
 6600 Autorefractor was the second commercial autorefractor
(1969).
 Munnerlyn (1978) design using a best contrast principle with
moving gratings led to the Dioptron, an automated objective
refractor.
OBJECTIVE SUBJECTIVE
SOURCE OF LIGHT
TIME REQUIRED
Infra-red light
2-4 min
Visible light
4-8 min
INFORMATION PROVIDED Less informative More informative (corrected
visual acuity)
PATIENT CO-OPERATION Required less (only
has to look straight at
target)
More co-operation (patient
has to turn knob, focus
target, answer questions
about appearance of target)
OCULAR FACTORS Better in macular
diseases with clear
ocular media
Can be done in hazy ocular
media
OVER REFRACTION
CAPABILITY WITH
SPECTACLES, CL, IOL
Difficult No problem
EXPECTED RESULTS Preliminary refractive
findings
Gives refined subjective
result.
TOPCON
RM 8900/8800
Monitor
Control lever
with
measurement
switch
Forehead
rest
Chin rest
Examination
window
Power
switch
1.Print switch
2.Menu switch
3.IOL switch
SPECIFICATIONS AND
PERFORMANCE
OPTICAL PRINCIPLES
1. The Scheiner principle
2. The optometer principle
3. Retinoscopic principle
4. Knife edge principle
5. Ray- deflection princile
6. Image size principle
Basic design
 Infrared source (IR-LED)
 Fixation target
 Badal lens system
 Polarized beam splitter
 Light sensor
Autorefractors:
Primary and secondary source of electromagnetic
radiation:
 Primary- NIR (Near Infrared Radiation): 780-
950nm
 Efficiently reflected back from the fundus
 Essentially invisible to the patient
 Secondary- back scatter from the fundus
 Determine sphere power, cylinder power, and
cylinder axis
 Fixation target
Accomodation is most relaxed when target is-
 Of low spatial frequency
 Same as typically seen at distance
Nulling vs open-loop
measurement principle
 NULLING PRINCIPLE REFRACTOMETERS:
 Change their optical system until the refractive error
of the eye is neutralized.
 OPEN-LOOP PRINCIPLE REFRACTOMETERS:
 Makes measurements by analysing the
characteristics of the radiation exiting the eye
 Do not alter their optical system
ALLOWANCE
•NIR = 800-900nm
•The reflectance of the
fundus increases
towards the red end of
the spectrum
•Into the infra red,
there will be multiple
reflections of
scattered radiation
within the eye which
will degrade the image
•A 800-900nm will
create hypermetropia
of 0.75-1.00 DS
relative to 550nm
Basic Principle
Infrared light
Rotating
chopper
Badal
lens
To PC
Polarised
filter
Slit
imagemore minus 0 more plus
Slit
mask
Light
sensor
BADAL OPTOMETER:
Infrared light is collimated
passes through rectangular masks
housed in a
rotating drum
beam splitter
Optometer system
Moves laterally to find the optimal
focus of the slit on the retina
Optimal Focus:
Optimal focus is achieved when a peak
signal is received from the light sensor.
SCHEINER DOUBLE PIN-
HOLE
 The original Scheiner double pin-hole was invented in
the 16th century.
 In a clinical setting, the double pin-hole identifies the
level of ametropia in a subject by placing it directly in
front of the patient’s pupil
 In a myopic eye, the patient
sees crossed diplopic
images, whereas in
hyperopia, the patient sees
uncrossed images.
 Crossed and uncrossed
doubling can easily be
differentiated by asking the
patient which image has
disappeared, when either top
or bottom pin-hole is
occluded.
OPTOMETER PRINCIPLE
 Aim: to study the number of dioptres of correction on a
scale with fixed spacing when the light from the target on
the far side of the lens enter the eye with vergence of
different amounts-
 0
 -
 +
 The vergence of the light
in the focal plane of the
optometer lens is linearly
related to the displacement
of the target.
Modern optometers
 Limitations of early optometers:
1. Alignment problem: both pin-hole apertures
must fit within the pupil.
2. Irregular astigmatism: the best refraction over
the whole pupil may be different in contrast to
the two small pin hole areas of the pupil.
3. Accommodation: the instrument myopia alters
the actual refractive status of the patient.
Scheiner’s Principle:
 Two LEDs (light emitting diodes) are imaged
to the pupillary plane.
 These effectively act as a modified Scheiner pin-
hole by virtue of the narrow pencils of light
produced by the small aperture pinhole located
at the focal point of the objective lens.
2 LEDs imaged to the
pupillary plane
Ocular refraction
l/t doubling of LED if
refractive error is
present
Reflection of LEDs
from retina back out of the
eye
Reflection by a semi-
silvered mirror
Dual photodetectors
RETINOSCOPIC
PRINCIPLE
 Autoretinoscopes
 Source of optical train corresponds to streak
retinoscope.
 Source of light is drum rotating about a source of
NIR which produces incident rectangular beam.
 Neutralization is by badal optometer
 Unwanted reflexes filtered by polarization of
incoming NIR
 Meridional refractors
1. Autoretinoscope based on direction of fundus
streak motion are nulling refractors.
2. Autoretinoscope based on speed of fundus
streak motion are non nulling refractors.
BEST FOCUS
PRINCIPLE:
 Aim: to find the best focus of an image on retina
through the analysis of maximum contrast that
can be captured by autorefractor.
 Both meridional and nulling
 Neutralization is by badal optometer
 Filters unwanted reflexes by polarization
Knife-edge principle
 Aim: to evaluate the refractive uniformity of the lens.
 These are nulling autorefracors that are not meridional
 Based on principle of reciprocity
 All light returning through the system passes completely
back into the source.
 Theoretically, no light should escape past the knife-edge.
Knife edge principle
Foucault Knife edge test for an
emmetropic eye.
The reflex on the detector
moves over most of the surface
Knife edge test for myopic eye.
The motion of the reflex across the
detector provides information on the
nature of the refractive error.
The speed of the reflex describes
the magnitude of refraction
Ray deflection principle
 Aim: to measure
 Linear deflection of the fundus image in 3 or more
meridia at a fixed distance from the eye
 Angular deflection of rays
 Position of far point in those meridia trignometrically
 Open loop (non-nulling) meridional refractors
 Corneal reflexes removed by central aperture in the
plane
 Coaxial reflexes removed by polarization
Image size principle
 Aim: to measure the size of fundus image in 3 or more
different meridia and calculate the full refractive error on
the basis of ocular magnification or minification of the
image relative to emmetropia.
 Non nulling
 Detection system : fundus camera- CCD camera, video
imaging of the fundus reflex, analysis by sophisticated
computer programme
Conclusion
 Autorefraction is a valuable tool in
determining a starting point for refraction.
 Modern technology has resulted in
improvements in design, size, speed and
accuracy.
 There are primarily two principles utilised in
current autorefractors
 the Scheiner principle
 Retinoscopic principle.
 Improvements in target design (auto-fogging
distance targets and open view
autorefractors) attempt to relax
accommodation in patients.
 Autorefractor should not be used as the final
refractive correction without further
confirmation.
Objective refraction

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Objective refraction

  • 1. Company LOGO Dr Sneha Thapliyal OBJECTIVE REFRACTION
  • 2. CLINICAL REFRACTION Determines and corrects refractive errors Objective refraction Subjective refraction Essential in: Young children Mental disability Language difficulty Deaf or mute
  • 3. OBJECTIVE METHODS OF REFRACTION 1. Retinoscopy 2. Autorefractometry 3. Photorefraction 4. Electrophysiological method of objective refraction
  • 4. RETINOSCOPY/SKIASCOPY /SHADOW TEST  Objective method of finding out the error of refraction by means of retinoscope utilizing the technique of NEUTRALIZATION
  • 5. Far point concept  The far point of eye is defined as the point in space that is conjugate with the fovea when accomodation is relaxed.  Emmetropia: Parallel rays focus on fovea.  Retina conjugate with infinity.  Far point is at infinity.  Ammetropias: Parallel rays do not focus on retina.  Ammetropic eyes require a correcting lens to make retina conjugate with infinity, i.e., to move far point to infinity  Hyperopia: Deficient refractive power.  Parallel rays focus behind retina.  Far point is beyond infinity.  Plus lens converges rays on to retina and conjugate fovea with infinity.
  • 6. Far point concept  Myopia: Excessive refractive power.  Parallel rays focus in front of retina.  Far point is between infinity and eye.  Minus lens diverges rays on to the retina and conjugate fovea with infinity.  Aspherical ammetropias:  This indicates different types of astigmatism.  This type of errors have two far points.  As a set of rays converge at one place and other at different place due to cornea not having same radius of curvature in all the meridians.
  • 7. Principle of retinoscopy:  To bring the far point of patient at the nodal point of the observer at the working distance
  • 8. NEUTRALIZATION 1. No movement of red reflex = NEUTRAL POINT 2. Reversal with overcorrection by 0.25 D 3. On alternating the working distance, slight forward, ‘with’ movement and an ‘against’ movement by slight backward movement.
  • 10. PREREQUISITES FOR RETINOSCOPY 1. Dark room: 6 m long 2. A trial set:  64 pairs of Spherical lenses(plus and minus) 0.12D 0.25-4.0D 4.0-6.0D 6.0-14D 14-20D 0.25 0.51D2D
  • 11. 20 pairs of Cylindrical lenses (plus and minus) 0.25-2.00D 2.0-6.0D 10 Prisms: ½ to 6 8,10,12 0.250.5
  • 12.  Accessories: Plano lenses Opaque discs Pinhole Stenopaeic discs Maddox rods Red and Green glasses
  • 13. 3. A trail frame  Light weight  Aluminium alloy- 30 g  Adjustable- horizontally and vertically  3 compartments: spherical, cylindrical, prisms  Cylindrical compartment : smooth and accurate rotation  Side pieces should be joint- tilted while testing for near vision  Back lens in trial frames should occupy as nearly as possible the position of spectacle lens i.e. around 12 mm in front of the cornea. 4. Phoropter or refractor  Turn the dial – change the lens before the aperture of the viewing system
  • 14. 5. Distance-vision chart 6. Near vision charts 7. Retinoscope: Invented by Dr Jack Copeland REFLECTING (MIRROR) RETINOSCOPES Priestley-Smith’s mirror Plane mirror SELF-ILLUMINATED RETINOSCOPES Spot self-illuminous Streak retinoscope
  • 17. bulb
  • 19.  Observing the optics of retinoscope we find two main systems - Projection system: Light source Condensing lens Focusing sleeve Current source - Obsevation system: Peep hole RETINOSCOPE AND IT’S PARTS:
  • 20. The retinoscope: how it works?  PROJECTION SYSTEM: illuminates the retina  Light source: a bulb with linear filament that projects a line or streak of light  Condensing lens: focuses rays from bulb onto the mirror  Mirror : placed in the head of instrument at 45 degree angle, it bends the path of light at right angles to the axis of the handle
  • 21.  Focusing sleeve controls  Meridian:Turning the sleeve rotates the streak of light.  Vergence:By varying the distance between the lens and the bulb  Bulb: Moved up-Plane mirror effect(Parallel rays) Moved down-Concave mirror effect(converging rays)  Lens: Moved up-Concave mirror effect Moved down-Plane mirror effect
  • 22.  In Copelands instrument,  moving the sleeve up or down moves the bulb.  Sleeve up creates plane mirror effect & sleeve down creates concave mirror effect Copeland type- fixed lens with moving bulb
  • 23.  In other Retinoscopes,  the lens rather than the bulb moves on moving the sleeve  Sleeve up creates a concave mirror effect & sleeve down creates plane mirror effect Fixed bulb type, the lens moves
  • 24.  OBSERVATON SYTEM:  Allows to see the retinal reflex  Light reflected by the illuminated retina enters the retinoscope, passes through an aperture in the mirror & out of the peephole at the rear end of the head.
  • 25. Optics in Retinoscopy  Illumination stage: light is directed into the subject’s eye to illuminate the retina  Reflex stage: image of the illuminated retina is formed at subject’s far point  Observation stage: image of the far point is located by moving the illumination across the fundus and noting the behavior of the luminous reflex seen by the observer in the subject’s pupil
  • 26. Clinician So S1 S2 Patient The light in the pupil is called the “ret reflex”
  • 28. Observer Subject Reflex disappears Reflex moves down, i.e. with direction of movement of light Mirror tilts further forwards Mirror tilts forwards S2 S2 Far point behind observers pupil Within pupil Outside pupil No S2 S1 Far point behind observers pupil. With movement of reflex, gradual change from red reflex to no reflex
  • 30. Observer Subject Far point in front of observers pupil Reflex disappears Reflex moves up, i.e. against direction of movement of light Mirror tilts forwards Mirror tilts further forwards S2 S2 Within pupil Outside pupil No S2 S1 Far point in front of observers pupil. Against movement of reflex, gradual change from red reflex to no reflex
  • 32. Reflecting mirror:  Perforated mirror  Central hole: 2.5mm anteriorly 4 mm posteriorly  By a plane mirror, rays are slightly divergent causing less illumination  Small hole corresponding to the central hole reduces illumination in pupillary area by causing central dark patch  Sides of the small hole are blackened to prevent annoying reflexes from entering the eye  Slightly concave mirror with central opening of 4mm and focal length greater than the distance between observer and patient; 150 cm
  • 33. LUMINOUS RETINOSCOPE  Streak retinoscope is the most popular  Both light source and mirror are incorporated  Intensity and type of beam can be controlled.
  • 34.  Two main techniques of retinoscopy are Static Retinoscopy:  It is the refractive state determined when patient fixates an object at a distance of 6 m with accomodation relaxed. Dynamic Retinoscopy:  The refractive state is determined while the subject fixates an object at some closer distance, usually at or near the plane of retinoscope itself with accommodation under action. RETINOSCOPY TECHNIQUES:
  • 35. PROCEDURE OF RETINOSCOPY  Patient is made to sit at a distance of 2/3rd of a meter  Accomodation should be relaxed  Use right eye for patient’s right eye and left eye for left  Trial frame is fitted  Direct the light from retinoscope into patient’s pupil  Move the retinoscope in horizontally and observe the red reflex.
  • 36.  Suitable lens is placed before the eyes to neutralize the band when the pupil will be filled with uniform light  Now move vertically, if still pupil is filled with uniform light, no astigmatism. Examiner sits just enough to the side to avoid blocking patient’s fixation
  • 37. Characteristics of the moving retinal reflex Speed and brilliance Low refractive High refractive Bright Faint Moves rapidly Moves slowly
  • 38. 2.Width of reflex Narrow Wide High degree of ametropia Low degree of ametropia 3. Presence of astigmatism When the axis does not correspond with the movement of the mirror, the shadow appears to swirl around.
  • 39. Examiner should scope both vertical and horizontal meridian. We correct the astigmatism with cylindrical lens. Cylindrical lens may be plus or minus, but have power in only one meridian, that which is perpendicular to the axis of the cylinder. The axis meridian is flat and has no power. ASTIGMATISM
  • 40. CYLINDRICAL AXIS  Break in the alignment between the reflex in the pupil and the band outside it when the streak is off the axis  Rotate the streak until the break disappears  Width of the streak appears narrowest when the streak aligns with the true axis.
  • 41. STRADDLING  Confirmation of axis  Retinoscope streak- 45 degree off axis in both directions  Correct axis- width of streak equal in both positions  Axis not correct- width is unequal  Narrow reflex is guide towards which cylinder’s axis should be turned
  • 42. PROBLEMS IN RETINOSCOPY: 1. Red reflex may not be visible or maybe poor  Small pupil  Hazy media  High degree of refractive error  Overcome by causing mydriasis and/or use of converging light with concave mirror retinoscope 2. Changing retinoscopic findings  Abnormally active accomodation  Overcome by fogging retinoscopy and cycloplegic 3. Spherical aberrations  Dilated pupils
  • 43. 4. Conflicting shadows  Irregular astigmatism 5. Triangular shadows  Conical cornea
  • 45. Cycloplegics in retinoscopy  When retinoscopy is performed after instilling cycloplegic drugs it is termed as Wet Retinoscopy 1. Atropine 1% ointment  Used in children < 7yrs age  Dose:1% eye ointment 3times daily for 3days  Effect lasts for 10-20days  Deduction for cycloplegia with atropine is 1D
  • 46. 2. Homatropine 2% drops  Used in hypermetropes between 7 to 35yrs  Dose:1drop instilled every 10mins for 6times & retinoscopy is performed after 1-2hrs  Effect lasts for 48-72hrs  Deduction for cycloplegia with homatropine is 0.5D 3. Cyclopentolate I% drops  Used in persons between 7 to 35yrs  Dose:1drop instilled every 10mins for 3 times & retinoscopy is performed after 1- 1 1/2hrs  Effect lasts for 6 to 18hrs  Deduction for cycloplegia with Cyclopentolate is 0.75D
  • 47.  Only mydriatic [ 10% phenylephrine] may is used in elderly patients to enhance the pupillary reflex when the pupil is narrow or media is slightly hazy  Later it should be counteracted by use of miotic drug[ 2% pilocarpine]
  • 48. Clinician S2 Patient We now have neutral We have also introduced negative vergence due to our working distance (WD) = 1/d (m) Where d = distance in m, measured between your ret and patient’s eye We have added lenses To get the right prescription we need to compensate Rx = lens power – 1/d So to get neutral, we needed: lens power = Rx + 1/d
  • 49. Working distance compensation Calculation  For example, if neutrality is achieved with a +3.00DS lens and your working distance is 50cm  Rx = +3.00DS – (1/0.50)  = +3.00 – 2.00  =+1.00DS Working distance lens  Before you begin, add a “working distance lens”  A +ve lens to cancel out the negative vergence  As in eg., WD = 50cm  WD lens = 1/0.50 = +2.00DS  Neutrality for the same patient is still +3.00DS  WD lens = +2.00DS  Lens power = +1.00DS Rx = lens power - 1/d
  • 50. AUTOREFRACTOMETRY Alternative method of assessing error of refraction by use of an optical equipment called refractometer or optometer OBJECTIVE SUBJECTIVE
  • 51. History  Collins(1937) developed the first semi automated electronic refractionometer.  Safir (1964) automated the retinoscope and this work led to the first commercial autorefractor-the Ophthalmometron.  6600 Autorefractor was the second commercial autorefractor (1969).  Munnerlyn (1978) design using a best contrast principle with moving gratings led to the Dioptron, an automated objective refractor.
  • 52. OBJECTIVE SUBJECTIVE SOURCE OF LIGHT TIME REQUIRED Infra-red light 2-4 min Visible light 4-8 min INFORMATION PROVIDED Less informative More informative (corrected visual acuity) PATIENT CO-OPERATION Required less (only has to look straight at target) More co-operation (patient has to turn knob, focus target, answer questions about appearance of target) OCULAR FACTORS Better in macular diseases with clear ocular media Can be done in hazy ocular media OVER REFRACTION CAPABILITY WITH SPECTACLES, CL, IOL Difficult No problem EXPECTED RESULTS Preliminary refractive findings Gives refined subjective result.
  • 53. TOPCON RM 8900/8800 Monitor Control lever with measurement switch Forehead rest Chin rest Examination window Power switch 1.Print switch 2.Menu switch 3.IOL switch
  • 55. OPTICAL PRINCIPLES 1. The Scheiner principle 2. The optometer principle 3. Retinoscopic principle 4. Knife edge principle 5. Ray- deflection princile 6. Image size principle
  • 56. Basic design  Infrared source (IR-LED)  Fixation target  Badal lens system  Polarized beam splitter  Light sensor
  • 57. Autorefractors: Primary and secondary source of electromagnetic radiation:  Primary- NIR (Near Infrared Radiation): 780- 950nm  Efficiently reflected back from the fundus  Essentially invisible to the patient  Secondary- back scatter from the fundus  Determine sphere power, cylinder power, and cylinder axis
  • 58.  Fixation target Accomodation is most relaxed when target is-  Of low spatial frequency  Same as typically seen at distance
  • 59. Nulling vs open-loop measurement principle  NULLING PRINCIPLE REFRACTOMETERS:  Change their optical system until the refractive error of the eye is neutralized.  OPEN-LOOP PRINCIPLE REFRACTOMETERS:  Makes measurements by analysing the characteristics of the radiation exiting the eye  Do not alter their optical system
  • 60. ALLOWANCE •NIR = 800-900nm •The reflectance of the fundus increases towards the red end of the spectrum •Into the infra red, there will be multiple reflections of scattered radiation within the eye which will degrade the image •A 800-900nm will create hypermetropia of 0.75-1.00 DS relative to 550nm
  • 61. Basic Principle Infrared light Rotating chopper Badal lens To PC Polarised filter Slit imagemore minus 0 more plus Slit mask Light sensor
  • 62. BADAL OPTOMETER: Infrared light is collimated passes through rectangular masks housed in a rotating drum beam splitter Optometer system Moves laterally to find the optimal focus of the slit on the retina
  • 63. Optimal Focus: Optimal focus is achieved when a peak signal is received from the light sensor.
  • 64. SCHEINER DOUBLE PIN- HOLE  The original Scheiner double pin-hole was invented in the 16th century.  In a clinical setting, the double pin-hole identifies the level of ametropia in a subject by placing it directly in front of the patient’s pupil
  • 65.  In a myopic eye, the patient sees crossed diplopic images, whereas in hyperopia, the patient sees uncrossed images.  Crossed and uncrossed doubling can easily be differentiated by asking the patient which image has disappeared, when either top or bottom pin-hole is occluded.
  • 66. OPTOMETER PRINCIPLE  Aim: to study the number of dioptres of correction on a scale with fixed spacing when the light from the target on the far side of the lens enter the eye with vergence of different amounts-  0  -  +  The vergence of the light in the focal plane of the optometer lens is linearly related to the displacement of the target.
  • 67. Modern optometers  Limitations of early optometers: 1. Alignment problem: both pin-hole apertures must fit within the pupil. 2. Irregular astigmatism: the best refraction over the whole pupil may be different in contrast to the two small pin hole areas of the pupil. 3. Accommodation: the instrument myopia alters the actual refractive status of the patient.
  • 68. Scheiner’s Principle:  Two LEDs (light emitting diodes) are imaged to the pupillary plane.  These effectively act as a modified Scheiner pin- hole by virtue of the narrow pencils of light produced by the small aperture pinhole located at the focal point of the objective lens.
  • 69. 2 LEDs imaged to the pupillary plane Ocular refraction l/t doubling of LED if refractive error is present Reflection of LEDs from retina back out of the eye Reflection by a semi- silvered mirror Dual photodetectors
  • 70. RETINOSCOPIC PRINCIPLE  Autoretinoscopes  Source of optical train corresponds to streak retinoscope.  Source of light is drum rotating about a source of NIR which produces incident rectangular beam.  Neutralization is by badal optometer  Unwanted reflexes filtered by polarization of incoming NIR  Meridional refractors
  • 71. 1. Autoretinoscope based on direction of fundus streak motion are nulling refractors. 2. Autoretinoscope based on speed of fundus streak motion are non nulling refractors.
  • 72. BEST FOCUS PRINCIPLE:  Aim: to find the best focus of an image on retina through the analysis of maximum contrast that can be captured by autorefractor.  Both meridional and nulling  Neutralization is by badal optometer  Filters unwanted reflexes by polarization
  • 73. Knife-edge principle  Aim: to evaluate the refractive uniformity of the lens.  These are nulling autorefracors that are not meridional  Based on principle of reciprocity  All light returning through the system passes completely back into the source.  Theoretically, no light should escape past the knife-edge.
  • 74. Knife edge principle Foucault Knife edge test for an emmetropic eye. The reflex on the detector moves over most of the surface Knife edge test for myopic eye. The motion of the reflex across the detector provides information on the nature of the refractive error. The speed of the reflex describes the magnitude of refraction
  • 75. Ray deflection principle  Aim: to measure  Linear deflection of the fundus image in 3 or more meridia at a fixed distance from the eye  Angular deflection of rays  Position of far point in those meridia trignometrically  Open loop (non-nulling) meridional refractors  Corneal reflexes removed by central aperture in the plane  Coaxial reflexes removed by polarization
  • 76. Image size principle  Aim: to measure the size of fundus image in 3 or more different meridia and calculate the full refractive error on the basis of ocular magnification or minification of the image relative to emmetropia.  Non nulling  Detection system : fundus camera- CCD camera, video imaging of the fundus reflex, analysis by sophisticated computer programme
  • 77. Conclusion  Autorefraction is a valuable tool in determining a starting point for refraction.  Modern technology has resulted in improvements in design, size, speed and accuracy.  There are primarily two principles utilised in current autorefractors  the Scheiner principle  Retinoscopic principle.  Improvements in target design (auto-fogging distance targets and open view autorefractors) attempt to relax accommodation in patients.  Autorefractor should not be used as the final refractive correction without further confirmation.