The globe effect, also known as rolling ball effect, is an optical illusion which can occur with optical instruments used visually, in particular binoculars or telescopes. If such an instrument is rectilinear, or free of rectilinear distortion, some observers get the impression of an image rolling on a convex surface when the instrument is panned.
Origin of the globe effect
The cause of the globe effect has been related to a non-vanishing barrel distortion generated in the process of visual perception: Already Helmholtz had constructed pincushion-distorted checkerboard patterns that he claimed to appear regular when viewed from a certain distance. More recently, systematic studies investigated the barrel distortion of human perception in test subjects and found that it is subject to a high statistical variance, i. e. varying greatly from individual to individual. The average degree of distortion is about half of the value suggested by Helmholtz, so that a large proportion of viewers are likely to perceive only an incomplete compensation of the bent edges in the Helmholtz checkerboard. The perceptual barrel distortion is sufficiently small to be unnoticeable in everyday life. However, if a rectilinear magnifying optical instrument is panned over a flat motif, the image pixels pass in front of the eye in rapid succession and the visual barrel distortion becomes visible as an apparent convex curvature of the image. This optical illusion remains hidden to the unarmed eye when turning the head, because it is prevented by the vestibulo-ocular reflex.
Formal Description
The image of an afocal optical instrument is distortion-free if the f-tan theta condition, also known as tangent condition and first defined by Bow and Sutton in 1861, is satisfied:
tan a = m tan A . ( 1 ) {\displaystyle \tan a=m\tan A.\qquad (1)}
Here, a {\displaystyle a} is the beam inclination with respect to the optical axis on the image side, and A {\displaystyle A} the beam inclination on the object side (or: subjective viewing angle of the image in the eyepiece and the inclination of the object with respect to the viewing direction), and m {\displaystyle m} is the magnification of the instrument. This relationship applies to all directions, so that the image is centrally symmetrical. To obtain a convenient parameterization of the degree of distortion, we introduce the general relationship
tan ( k a ) = m tan ( k A ) , ( 2 ) {\displaystyle \tan(ka)=m\tan(kA),\qquad (2)}
with the distortion parameter k ∈ [ 0 , 1 ] {\displaystyle k\in [0,1]} . This yields the f-tan theta condition (1) in the special case k = 1 {\displaystyle k=1} . The case k = 0.5 {\displaystyle k=0.5} is known as the circle condition and provides the pincushion-distorted pattern which was implemented by Helmholtz in his checkerboard. Yet another limit case with k → 0 {\displaystyle k\rightarrow 0} leads to the f-theta condition (also known as angle condition)
a = m A , ( 3 ) {\displaystyle a=mA,\qquad (3)}
which produces a considerably stronger pincushion distortion. The meaning of the infinite set of curves spanned by the distortion parameter is thus clear: Starting with the value 1, a reduction of k {\displaystyle k} produces an increasingly stronger pincushion distortion, which reaches its highest value at k = 0 {\displaystyle k=0} . At this point, another distortion is needed, which originates from the observer's visual perception. For this purpose, perceptual psychology introduces an abstract visual space whose properties are defined by mathematical modeling. In order to create a barrel distortion of varying strength, we define
y = l − 1 tan ( l a ) , ( 4 ) {\displaystyle y=l^{-1}\tan(la),\qquad (4)}
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