The side view of a lens in Figure 2 shows a simplified representation of a conventional machine-vision lens.
All imaging lenses have an aperture stop, a physical device that limits the amount of light energy that can pass through the lens, or a group of lenses. In a conventional lens, the opening or closing of the aperture stop changes the overall brightness of the image across the entire image, without affecting the size of the image. In your eye, the iris forms the aperture stop.
In addition, all lenses contain pupils. Specifically, every lens has both an entrance and exit pupil. The entrance pupil is the image of the aperture stop in object space, and the exit pupil is the image of the aperture stop in image space. That is, the entrance pupil is the image of the aperture-stop image as you would see it viewed from the object side of the lens. The exit pupil is the aperture-stop image as you would see it if viewed from the image side of the lens.
A lens diagram such as the one shown in Figure 2 typically includes three rays drawn from any point on the object through the lens to the image. The chief, or principal, ray passes obliquely through the center of the aperture stop. The two remaining rays, called marginal or paraxial rays, are drawn to coincide or come close to the edges of the aperture. They represent the outside limits of the “bundle” of light rays that pass through an optical system of one or more lenses.
The diagram in Figure 2 shows the paths of three light rays that start at a real object—in this case, the tip of an arrow. The three rays trace light paths through the lens to finally produce a corresponding point on the image. When all the rays that pass through a lens converge in a plane, they produce an image.
In most conventional lenses the aperture stop is located within the lens assembly. The images of the aperture stop, that is, the entrance or exit pupils, are made up of converging light rays. In a telecentric lens, the aperture stop is located at the focal point of the lens. Due to this unique posit ion of the aperture stop, the light rays that form the images of the aperture stop travel parallel to the optical axis and are considered to be located at infinity.
If you were to look through a telecentric lens from the object side, for example, you would see the entrance
pupil of the lens. The same is true with a conventional lens. On first observation the pupils may look the same. For the telecentric lens. Your eye focuses at infinity, and the entrance pupil of the lens remains in focus with no further refocusing of your eye as you move the lens closer or farther. On the other hand, with a conventional lens, your eye would need to refocus on the image of the entrance pupil as you move the lens closer or farther away. The fact that the entrance or exit pupil is located at infinity means that the principal ray is parallel to the optical axis of the lens. This characteristic is what defines a telecentric lens.