jars.com  Ophthalmic Optics for beginners



The aim of this page is to explain some basic concepts about ophthalmic optics in order to understand the idea of the above applet. Of course you can try it without any knowledge of optics but it would be better to have a look at the following lines to discover (if you are not a specialist) a subject at the frontier between optics and physiology.

I wish to thank A.Meyer (Science &Vie) for the eye's illustration and Caroline, my English teacher, for checking the English language of this page.
 

The eye : how does it work ?


Human eye

The light emitted by the object you are looking at enters the eye through the cornea. The light rays then pass through the pupil (which regulates the amount of light entering the eye) and then cross the (crystalline) lens. Finally, the light rays are focused on the retina which is a thin layer covered with light receptor cells. Thanks to electrochemical reactions, the light is converted into electrical impulses transmitted to the brain by the optic nerve.

About at the center of the retina is a small depression known as the macula. At the center of the macula, in an area called fovea, cells are densely packed and provide the sharpest colored and most detailed information. But, despite the importance of the fovea, the other parts of the retina are also very useful to detect motion, to see in dim light ...

From an optical point of view, the eye may be compared to a camera. On the one hand, the lens combination of the camera forms an image on the sensitive film and on the other hand, the eye forms an image on the retina.

An eye is said to be normal or emmetropic if the image of a distant object falls on the retina :

Emmetropic eye
otherwise the eye is said to be ametropic.

But the normal eye is also able to see near objects thanks to a fine focusing mechanism, known as accommodation. Through changes in its shape, the (crystalline) lens gives a variable focal length to the eye. With this accommodation mechanism, the normal young human eye is able to see near objects, say 25 cm in front of him. In this way, the human eye may be more precisely compared to an autofocus camera, adjusting continuously in order to bring the image into focus.

But with age, accommodation begins to fail and the image of near objects can't be focused on the retina : the increase of power produced by the accommodation is not important enough. This phenomena is known as presbyopia and begins to affect people at the age of 40.


Ametropia



We are going to consider two kinds of ametropia : myopia and hyperopia. Note that we suppose the eye to be in relaxed condition, that is to say, accommodation not in use.

Nearsightedness, short-sightedness or myopia

Myopic eye
Myopia is the condition in which the image of a distant object falls in front of the retina. This occurs when the axial length of the lens is too large for the power of the lens system.

Farsightedness, long-sightedness or hyperopia

Hyeperopic eye

Hyperopia is the condition in which the image of a distant object falls behind  the retina. This occurs when the axial length of the lens is too short for the power of the lens system.

Why ophthalmic lenses ?


There are different means to correct ammetropia as contact lenses, refractive surgery, laser procedures, but the oldest and non invasive one is to wear ophthalmic lenses.

Correction of myopia

Myopic eye corrected

One way to correct myopia is to place a negative lens (or diverging lens) in front of the eye.

Correction of hyperopia

Hyperopic eye corrected

One way of treating hyperopia is to place a positive lens (or converging lens) in front of the eye.
 

This is the task of your optometrist to define the characteristics of the lenses you need to wear : the prescribed lenses.
One common way to characterize this prescribed lens is to give its vertex power. Let's have a look at the definition of the vertex power of a lens :

Definition of the vertex power

As you know, for an object at infinity, the image is formed in f' : image focus point. By definition, the vertex power of a lens is the inverse of the distance between the vertex of the rear surface and f'. This quantity is given in m-1 or diopter (D).
For example, in the case of myopia you may need a -3 D diverging lens, or a +3 D converging in the case of hyperopia.

Let's now suppose an emmetrope person. At this point, he can clearly see objects at different distances, but only objects which are just in front of him. If the object he is looking at moves in the field of vision, what happens ?

In the field of vision
As you can see, the image of the object being viewed, doesn't fall on the fovea and the vision is not perfect (without a good acuity). To get round this problem, one can imagine different solutions.

First, you can move the object (as a jeweller looking at a diamond) or turn around it, in order to put it just in front of your eye. Of course, this may not always be very easy, particularly if you are looking at stars in the sky. Another simpler and common way is to move the head or to turn the eyes (or both). In the following we will only consider motion of the eyes, for a given position of the head :

Rotation of the eye
In fact the eyeball is continuously moving, so that light emitted by object of primary interest falls on the fovea. For example, when you are reading a newspaper, it is impossible to read an entire line without moving the head or the eyes because this task requires a good acuity.

A schematic representation of the eye is as follows. The eyeball rotates around a fixed point known as Eye's Center of Rotation (ECR), in order to focus image on the fovea. This is obtained when the (main) light ray passes through the center of the pupil and through the eye's center of rotation, defining in this way a position of gaze.

Position of gaze

However, what does it mean for the wearer of ophthalmic lenses ?


Vision through ophthalmic lenses



When a myope or hypermetrope looks through a lens, thinks are a little bit different. First, due to the Snell-Descartes laws, the rays of light don't cross the lens in a straight line.
 
Myopic eye and diverging lens Hyperopic eye and converging lens
Myopic eye and diverging lens Hyperopic eye and converging lens
As you can see, for the same position of gaze, emmetrope, myope and hypermetrope will not see the same object, or in other words, a myope's eye will rotate less than an hypermetrope's eye to see the same object in the field of vision. This is the reason why myopes may wear small frames and they are lucky because the diverging lenses they need generally have an important and ungracious edge thickness.
This phenomena is known as distortion.

But at this time there is a last problem : ophthalmic lenses provide a good vision only while one looks through their centers. This is not the case as the position of gaze is non null, and the vision may be affected. One way to quantify the quality of vision would be to analyze the image formed on the retina. But, on the one hand, it is difficult to make ray tracing inside the eye because of it's complex structure and, on the other hand, it is not easy to interpret how the brain "sees" this image. How to avoid this ?

We are going to analyze the image formed by the lens because, in fact, this is the image the eye is looking at : one speak about virtual image. But one thing is sure : the best the image produced by the lens, the best the quality of vision for the wearer.

For a null position of gaze, we know that the image formed by the prescribed lens must be at a distance 1/D m from the vertex of the back surface. By extension for the other positions of gaze, and because of the rotational symmetry around the ECR, the image should be formed on a sphere centered on ECR,  and known as far point sphere.

Focus on the far point spehere

As you can imagine, the image formed by the lens is not always perfectly focused on the far point sphere. One way to know if the image is exactly positioned, is to measure the distance between the intersection of the ray with the vertex sphere (which a sphere centered on the ECR and tangent to the back surface) and the focus point. This quantity is defined for each position of gaze and should always be 1/D m.


Aberrations introduced by the ophthalmic lenses



Of course, this is not the goal of the lens to introduce aberrations which will be directly  perceived by the wearer and will decrease the acuity, but  things are things ... However, despite theses aberrations, be confident that ophthalmic lenses are well appraised by the wearers.

Two kinds of aberrations may deteriorate the image :

We are going to consider two of the principal monochromatic aberrations taken into account in the context of the ophthalmic optics : power error and astigmatism.
  As explained before, for a given position of gaze, the focus point may be in front, on, or behind the far point sphere. Power error is just the difference between the power produced by the lens and the prescribed power. Power error is positive if the power produced by the lens is more than D (the prescribed power), and negative (or null) otherwise.
  Very simply, astigmatism is due to the fact the incident cone of rays strikes the lens asymmetrically. When the cone of rays sent by the observed object lies an appreciable distance from the center of the lens, they don't focus in a single point but are imaged as two short lines, known as astigmatic foci. The red one is the tangential foci and the blue one the sagittal foci.

Astigmatism

This is a schematic view with the eye, the lens and the astigmatic foci :

Foveal vision model

Let's now define different quantities  :

and Astigmatism is always null at the center of the lens and generally increases with position of gaze. Power error is supposed null at the center of the lens, or in other words, we consider the lens has always the prescribed power at its center.

These quantities are defined for each position of gaze and can be represented on such a graph :

Astigmatism and power error

How to read this graph ?
The red, blue and black curves represent respectively the tangential power, the sagittal power and the mean power of a +9 D ophthalmic lens. In this case, and for a 25° position of gaze, T > 9 D, S < 9 D and (T+S)/2 > 9 D. Power error which is the difference between the mean power and the prescribed power (9 D) is greater than 0, and can bee red on the horizontal axis, scaled between -1 D and +1 D. Astigmatism can be evaluated as the horizontal distance between the T and S curves. Power error and astigmatism are also printed in green for the current position of gaze.


Applet



This applet lets you modify the different parameters defining the lens, and observe the consequences on the performances in term of power error and astigmatism. It has been tested and works fine with Internet Explorer 5.0 and Netscape Communicator 4.6.

Image of the applet

Eight parameters may be modified :


There are 2 different ways to run this applet.


Documentation of the program


Just a short "javadocumentation" (in french) about the program : javadoc
 


A few  links


Everything about the java language
http://java.sun.com

Everything you want to know about the eye
http://webvision.med.utah.edu/

A lot of interesting links about optics
 http://members.xoom.com/joelzahn/lightoptics/index.html

American Optometric Association
 http://www.aoanet.org/

A nice animation
 http://www.vision1to1.com/
 


Copyright © 1999-2000 Baudartum Communications Corporation.