Relative Mag
Spectacle Mag
Compares retinal image size corrected vs. uncorrected
SM = lglasses/luncorrected
Image size with glasses/image size without glasses
SM for thick lenses
SM = (shape factor) x (power factor)
Shape factor = 1/1-(t/n)F1
t: central thickness of lens (m)
n: index of refraction
F1: front surface power of lens
Power factor = 1/1-hFv
h: vertex distance (m)
Distance between back of lens and entrance pupil of eye (m)
Take entrance pupil distance to cornea to be 3 mm if not specified
To get h, add vertex distance to distance between pupil and cornea (3 mm), and convert to m
Fv: back vertex power of lens
Back vertex power is just the power of the lens
Equation should tell you front vertex power separately
Whatever you get when you multiply shape factor and power factor tells you how much bigger image is with specs
Ex: if shape factor x power factor = 1.31, image is 31% bigger with specs
For plus lenses:
Increasing vertex distance (h), thickness (t), and BC (F1) increases SM
Increasing n decreases SM
For minus lenses:
Increasing thickness and BC increases SM
Increasing vertex distance and n decreases SM
Increasing thickness and BC always increases SM
Increasing n always decreases SM
Increasing vertex distance increases SM in (+) lenses (why presbyopes pull lenses away from face) and decreases SM in (-) lenses
Relative Spectacle Mag (RSM)
Compares retinal image size corrected vs. retinal image size on an emetrope
Retinal image size corrected relative to standard eye
RSM = Ia/Is
Image size in an ametrope/image size in a standard eye
Standard eye is defined as a +60.00D emmetrope
Axial ametrope
Hyperopia: eye is too short
Myopia: eye is too long
Axial ametropes best corrected with glasses: Knapp’s Law
Knapp’s Law: RSM is 1 in an ametrope if a thin lens is placed at the primary focal point of the eye
Primary focal point for axial ametrope is about 15-17 mm in front of cornea
Explains why glasses work better for axial ametropes (they correct for the length of the eye)
Refractive ametrope
Best corrected with contact lenses
Uncorrected refractive ametropes all have the same retinal image size whether they are hyperopic, myopic, or emmetropic (same length of the eye)
Need CLs to make sure the mag of the image remains constant even with optical correction for the refractive error
CLs have a small vertex distance (h) and thickness (t), so they don’t effect image magnification very much
Retinal Image Size
Uncorrected axial ametropes
Retinal image size: myopes > emmetropes > hyperopes
Axial myopes have largest retinal image size (long eye)
Corrected axial ametropes
Specs at the primary focal point of the eye give RSM = 1
CLs on axial ametropes don’t correct for retinal image size
Uncorrected refractive ametropes
Hyperopes and myopes have the same retinal image size as emmetropes
Corrected refractive ametropes
CLs don’t change the retinal image size, RSM = 1 in all refractive ametropes
Specs give a magnified retinal image size for hyperopes (+ lens) and minified retinal image size for myopes (- lens)
If one eye is +1.00 and one eye is -1.00, the +1.00 lens will have more SM (+ induces mag)
Make the (-) lens thicker and steeper or the (+) lens thinner and flatter to even out SM
Aniseikonia: difference in size or shape of retinal images seen by left and right eyes (anatomical or induced)
Anatomical aniseikonia: difference in retinal images due to anatomical asymmetry, like discrepancy in photoreceptor density
Induced aniseikonia: difference in retinal images due to optics of vision correction, like differences in spectacle mag in Spec Rx
Overall aniseikonia: difference in image size between the two eyes effecting the entire field
Meridional aniseikonia: difference in image size between the two eyes due to difference in cylinder, causing the effect to be prominent in only one meridian
Can cause a straight line to look tilted
Prescribing
Small differences in RSM: give equal BCs and equal thickness
Large differences in RSM: give the eye with the highest RSM a flatter, thinner lens
Increased BC and increased thickness increase RSM
Prescribe a thicker, steeper lens for the eye with the lower RSM
If one eye has a small Rx, and the other eye has an Rx over 4.00D, the ametropia is likely axial: prescribe specs
If one eye has a small Rx, and the other eye has an Rx under 4.00D, the ametropia is likely refractive: prescribe CLs
Aniseikonia from a large astigmatism is likely refractive/cornea-related: prescribe CLs
Every 1.00D power difference between the eyes gives 1% aniseikonia
Anisometropia
Refractive state of the left eye is different to the refractive state of the right eye, usually by more than 1.00D
Accommodation occurs equally in both eyes
Myopic patients will use the more myopic eye for near vision (accommodate less) and the less myopic eye for distance vision (see better at distance)
Myopic patients don’t need to accommodate for distance, and might not need to accommodate too much for near, so accommodation should not effect them too much
Hyperopic anisometropic patients will likely not see clearly at any distance, because they need to accommodate even at distance
Hyperopic patients will use the least hyperopic eye to accommodate at all distances (needs to accommodate less, but still overworking)
Puts kids at risk for amblyopia at early childhood
Patients that are hyperopic can still have good DV by accommodating to bring the image forward, but they may have eyestrain from the constant need to accommodate
NV requires hyperopic patients to bring the image even further forward, and they might not be able to accommodate enough to do that
Antimetropia: one eye is hyperopic and the other is myopic
Absorptive Lenses
When light passes through a lens, it is reflected by both surfaces (front and back), and absorbed by the lens material
Transmittance (t): measures the amount of light that gets through an optical system (0-1)
When light hits a lens it is lost in 2 ways: reflected at front and back surfaces, absorbed by lens material
To measure light reflected, use Fresnel’s law: reflection of light at the boundary between two media indices
R = (n2-n1/n2+n1)2
Use same number twice for front and back surface when looking for total transmittance (n2 is lens medium)
To convert Fresnel’s law to transmittance:
Ts = 1-R
Ts: transmittance at each surface
Need to do this for front and back surface
To measure light absorbed, assume the amount transmitted by the medium is 1 - amount absorbed by the medium:
TM = 1 - (amount of light absorbed by lens)
TM: transmittance through media
To find total transmittance (T):
T = (TS1)(TS2)(TM)
Ideal thin film: choose film material that minimizes reflection
nf = sqrt(n1nL)
nf: index of film
n1: index of initial medium (air)
nL: index of lens
Summary
Accommodation
Hyperopes accommodate less with CLs
Can need an add earlier
Myopes accommodate more with CLs
Magnification
Hyperopes have a smaller retinal image with CLs (less SM)
Myopes has a larger retinal image with CLs (less SM)
Vergence
Hyperopes converge less with CLs (less induced BO)
Myopes converge more with CLs (less induced BI)
CLs induce less prism
Prism in specs allows eyes to look in the direction with less work