ABO Basic Review
August 2nd, 2011
This is a review I did for the ABO
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August 2nd, 2011
This is a review I did for the ABO
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November 18th, 2009
One area of Opticianry that seems to have more Opticians baffled is prism. I hope in this short tutorial it will ease the misunderstanding of prism. …Continue
November 11th, 2009
When we compensate an Rx, we do so because the lens changes power as moves closer or farther away from the eye. We are making an Rx stronger or weaker depending on whether the lens is moved closer farther away.
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November 10th, 2009
1. The approximate power on the vertical meridian for the Rx +3.00 -1.50 x 102 is ______. Give the power rounded to two decimal places, not to 1/8 diopter steps.
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November 10th, 2009
1. If a polycarbonate lens (n = 1.586) is made with a front surface power of +10.25, a back surface power of -3.00, and a center thickness of 4 mm, what power will the lensmeter show? Give the power rounded to two decimal places, not to 1/8 diopter steps.
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June 22nd, 2009
Determining the correct lens blank is the first step to surfacing a lens. This is a two step process, the fist step is to find the correct base curve and the second step is to determine the needed blank size.
April 1st, 2007
The purpose of this article is to build on what was discussed inRay Tracing of Thin Lenses. If you have not read that article it would be wise to do so. This article assumes a basic understanding of mathematical concepts and an understanding of some optics.
Tracing a thick lens is different because the ray of light is going to be refracted at more than just one meridian. A Thick Lens is defined as a lens in which the separation between the two surfaces is too great to be ignored. For example the lens power measured from the front of the lens will be different than if it were measured from the back, due to the thickness.


A couple of points to note, all rays that are traced will be paraxial, close to the axis. Usually opticians tend to give a positive radius to the front curve and a negative radius to the back curve, because the powers are positive and negative respectively. We need to understand that a positive radius is defined as the center of curvature being to the right of the lens and a negative radius is when the center of curvature is to the left.


Since we are dealing with thick lenses we need to know where to measure the focal length, object distance, and image distance. We will not measure these items from the center of the lens or from the lens vertices’s, but rather from the principal planes (
). Principal planes are where refraction is assumed to occur
Now we need to find the equivalent power of the lens. The equivalent power is assigning one power to a two lens system. For example, if you read a thick lens in the focimeter on the front and then read the back there would be two different powers. The equivalent power is the position of the principal planes with respect to the first and second focal points. Once we find the equivalent power we can then find the principal planes.

We will explain in more detail later, just understand that
is measured from the front vertex and
is measured from the back vertex. Also understand that
and
are measured from
and
respectively.
Formulas to trace a thick lens
Radius of Curvature

is the radius of curvature in Meters
is the refractive index of the the refracting side of the surface
is the refractive index of the incident side of the surface
D is the power of the surface in Diopters
Front Vertex Power

is the front vertex power
is the power of the front of the lens
is the power of the back of the lens
is the thickness in Meters
is the refractive
Back Vertex Power

is the back vertex power
is the power of the front of the lens
is the power of the back of the lens
is the thickness measured in Meters
is the refractive index
Primary Focal Point (
)

is the primary focal point measured in Meters
is the front vertex power
Secondary Focal Point (
)

is the secondary focal point measured in Meters
is the back vertex power
Equivalent Power
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is the equivalent power
power of the front of the lens
power of the back of the lens
is the thickness measured in Meters
is the refractive index
Equivalent Focal Point(
)

is equivalent focal point measured in Meters
is the equivalent power
Image Distance

Linear Magnification

Image Height

Now we are armed with the information we need to trace a thick lens.
Example: A plastic( n = 1.50) lens with a thickness of 20mm is surrounded by air. It has a front power of +20.00D and a back power of -3.00D. If and object is placed 100mm in front of the lens where does the image form, how much magnification is present, and is the image inverted or erect. Find the principal planes, equivalent power, linear magnification, image distance, and image height.
Step
1: Find the radius of curvature for both surfaces.


* Note the refracting ray is in air and the incident ray is in the material
Step 2: Find the back and front vertex powers.


Step 3: Find the equivalent power.

Step 4: Find the primary, secondary, and equivalent focal points.



Now
we are ready to draw the lens, optical axis, principal planes,
,
and
.
First you need to draw the optical axis, grab a compass and draw
(25mm).

Second from the apex of the 1st surface
measure and draw a point that is equal to the thickness of your
lens(20mm) and with your compass draw
(167mm)
from that point.


Now that we have the lens drawn we need to mark our
primary focal point, secondary focal point, and our principal planes
on our optical axis.

We are now ready to finish drawing our optical axis,
but we need to know how long to draw it. We know that our object is
located -100mm from the front vertex, however we will measure it from
p1.
Take the difference between f1 to front vertex and p1 to
f1. Then subtract that number from your object distance.
-58 – (-56) = -2
-100 – (-2) = -98
-98 is the distance from p1 to your object or your
object distance. Now we will use our equivalent power to find the
image distance

So the image is located131mm from p2. Now let us find
linear magnification.

So now we will trace three rays to show that our image
ends up 131mm from p1, it will be inverted, and it will be magnified.
We know this because of the result of our linear magnification
formula.
