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Helmet-Mounted Displays: - USAARL - The - U.S. Army

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58<br />

William E. McLean<br />

given FOV. To demonstrate the importance and contribution of the eye<br />

clearance on FOV, recalculating the above equation with an eye clearance<br />

of 30 mm and the eyepiece and exit pupil the same, the FOV is reduced to<br />

23.3 degrees. Similarly, to obtain a 40 degree FOV with 30 mm of eye<br />

clearance, the diameter of the eyepiece would be 31.0 mm. Also note that<br />

reducing the exit pupil size reduces the eyepiece diameter the same amount.<br />

With angular eye movements, the eye is displaced perpendicular to the<br />

optical axis and will require the optical exit pupil to be located ideally<br />

approximately 2 to 3 mm behind the pupil of the eye, particularly for pupil<br />

forming imaging systems (Shenker, 1987).<br />

<strong>The</strong> primary purpose of this first order optical exercise was to show<br />

how the variables of FOV, exit pupil size, eye clearance, image source size,<br />

and f/# interact with the simplest of optical designs for a flat display with<br />

nonsee-through vision. When see-through vision is desired with an added<br />

combiner, the calculations become more complex, but can be solved with<br />

multiple trigonometry steps. <strong>The</strong> optical designer can also increase the<br />

FOV for a given eyepiece focal length by using a concave display or image<br />

plane, inducing barrel distortion for the objective lens and neutralizing the<br />

barrel distortion with an equivalent pincushion distortion for the eyepiece.<br />

This technique is used for ANVIS. Graphs of the diameter of the eyepiece<br />

for the various HMD designs will be shown in the next section for<br />

comparison purposes.<br />

Optical Aberrations<br />

In addition to just focusing or collimating the display, additional optical<br />

elements are usually required to compensate for chromatic and spherical<br />

aberrations, distortion, field of curvature, etc. Because the additional<br />

elements add undesirable mass to electro-optical devices, a short discussion<br />

of these optical characteristics will be included (Smith, 1990).<br />

Chromatic aberration<br />

All lens elements with refractive power act like a prism by refracting<br />

(bending) wavelengths of different colors by slightly different amounts. To<br />

compensate for this and to reduce the rainbow effects from the lens<br />

elements, the optical designer uses lenses in pairs (usually fused), opposite<br />

in lens power with different refractive characteristics (index of refraction<br />

and dispersion). <strong>The</strong>se lenses are called achromats. Other methods to<br />

reduce chromatic aberrations are to (a) use narrow band light sources or

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