From the fields of robotics, vision, and image processing, there is a demand for lenses without loss of sharpness, low distortion, and high residual brightness at short working distances.

1. Basic relationships of optical imaging 1.1 Explanations of simple imaging laws For the following simplified and therefore only approximately valid formulaic imaging relationships, the basic relationships depicted in the illustration should be considered with a positive numerical value. Although this does not correspond to the sign convention commonly used in optics, it is easier to handle for the present purpose.

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Fundamentals of lens selection at a glance As mentioned earlier, our lenses are used for various tasks in industrial image processing. The following information on the most important technical-optical fundamentals as well as the quality features of the lenses are intended to help the user select the most suitable lens for their

u⌀' Diameter of blur circle to be defined depending on the application. For example, for the 2/3" format, u⌀' = 30 μm makes sense.

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Extreme close-up Lenses are designed for a specific range of object distances, usually from infinity to a certain minimum object distance (MOD). For possibly required shorter focusing distances, the possible displacement (stroke) of the lens from the image plane for focusing is no longer sufficient. Here, two options are available to capture very close objects, with a loss in imaging quality expected.

User formulas a    Object distance = distance object-lens in mm (OH) y    Object size (half diagonal) in mm y'    Image size (half diagonal) in mm        for 1/2" format: 2 y' = 8 mm        for 2/3" format: 2 y' = 11 mm        for 1/A" format: 2 y' = 16 mm

av    Object width in front (in the direction of light) that is still sharply imaged ah   Object width in the rear (in the direction of light) that is still sharply imaged.

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a) With the help of an extension tube, the distance between lens and image can be increased. The length of the extension tube z' is determined by the focal length f' and the magnification β' (lens in position ∞):

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Focal length A ray near the optical axis originating from an infinitely distant object intersects the optical axis on the image side at the focal point F'. The distance of this focal point from the reference plane (principal plane) of the lens is the focal length f'. For the object side, f = -f' applies analogously.

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Object distance        1/2 inch sensor: 2 y' = 8 mm a = 1 m                         2/3 inch sensor: 2 y ' = 11 mm f' = 35 mm                  1 inch sensorr: 2 y' = 16 mm

Optical imaging An object of size y located at a distance of the object distance a in front of the lens is imaged by the lens onto the image plane, which is located at a distance of the image distance a' behind the lens. There, the image sensor of the camera is located. The image size is y'. The change in image size depending on the object size is determined by the Image scale

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b) With the help of a close-up lens, the object distance can be shortened. When setting the lens to infinity (∞), an object distance a is obtained in front of the close-up lens, which corresponds to the focal length. The reciprocal of this required focal length (= required adjustment distance a) gives the required refractive power D of the close-up lens, which is given in diopters (dpt = 1/m):

An object of size y = 2.6 m at a distance a = 4 m should be fully captured with a 2/3" camera (2y ' = 11 mm). What focal length of the lens is required?

Image angle The maximum extent of the object captured by the lens, starting from the reference plane of the lens, can be described by the image angle w. If the object is at infinity, the image is at the focal point F' of the lens. In this case, there is a simple relationship between the image angle w, the image size y', and the focal length f':

Aperture number The aperture number k is a measure of the illumination intensity (image brightness). It depends on the focal length f' and the diameter of the entrance pupil ⌀EP, which represents the image of the aperture in the object space. Looking from the front into the lens, you see the diameter EP. Thus,

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Discover the formulas that form the basis for the precision and performance of our lenses. Learn how these formulas shape our lens technology and drive our lenses for industrial image processing forward.

A 10 m large object (y = 5 m) should be fully captured with a 1/2" camera (y' = 4 mm) and a Schneider-Kreuznach 1.4/12 mm lens. How far must the camera be from the object?

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What solid angle must a lighting illuminate to obtain a uniformly bright image with a 2/3 camera (2y' = 11 mm) and a Schneider-Kreuznach 1.4/8 mm lens?