DK Eyewitness - Astronomy
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John dollond<br />
The English optician John Dollond<br />
(1706–1761) was the first to perfect the<br />
achromatic lens so that it might be<br />
manufactured more easily and solve<br />
the problem of chromatic aberration.<br />
Dollond claimed to have invented a<br />
new method of refraction.<br />
Chromatic aberration<br />
When light goes through an<br />
ordinary lens, each color in the<br />
spectrum is bent at a different angle,<br />
causing rainbows to appear around<br />
the images viewed. The blue end of<br />
the spectrum will bend more sharply<br />
than the red end of the spectrum,<br />
so that the two colors will focus at<br />
different points. This is chromatic<br />
aberration. By adding a second lens<br />
made from a different kind of glass<br />
(and with a different density), all<br />
the colors focus at the same point<br />
and the problem is corrected.<br />
Earth<br />
Light waves from a<br />
stationary star<br />
Light waves from star<br />
approaching Earth<br />
are compressed<br />
Rays<br />
of light<br />
Spectrum of star’s light<br />
Blue focus<br />
Lens<br />
Light waves from receding<br />
star are stretched<br />
Star<br />
Red focus<br />
Star<br />
Rays<br />
of light<br />
Both colors at<br />
same focus<br />
Two lenses<br />
An effect of light<br />
One effect of light viewed<br />
through a telescope can be<br />
explained by the Doppler effect.<br />
This explains how wavelength is<br />
affected by motion. The light of<br />
any object, such as a star approaching<br />
Earth, will be compressed and shifted<br />
toward the short wavelength (blue)<br />
end of the spectrum. Light from<br />
objects moving away from Earth will be<br />
elongated and shifted toward the red<br />
end of the spectrum. These effects are<br />
called “blue shift” and “red shift.”<br />
A refractor telescope<br />
In a refractor telescope, the convex objective lens<br />
(the one farthest from the eye) collects the light<br />
and forms an image. The convex eyepiece lens<br />
(the one closest to the eye) magnifies the image<br />
in just the same way as a magnifying glass.<br />
Galileo used a similar type of refractor telescope<br />
(p.20). The main problem with the refractor<br />
telescope is chromatic aberration (above).<br />
Viewer<br />
Eyepiece<br />
lens<br />
A reflector telescope<br />
Sir Isaac Newton (p.21) developed a version of the<br />
reflector telescope that consists of a large concave, or<br />
curved, mirror to catch the light. The mirror then sends<br />
the light back to an inclined flat, or plane, mirror where<br />
the image is formed. The eyepiece lens magnifies the<br />
image. Unlike the lenses in a refractor telescope, the<br />
mirrors in a reflector telescope do not cause chromatic<br />
aberration, so the image is clearer.<br />
Object<br />
Virtual image<br />
Convex lens<br />
Assumed path of<br />
light rays<br />
Light rays<br />
bend inward<br />
Convex objective lens<br />
Viewer<br />
How a lens magnifies<br />
When a convex lens is held between the eye and an<br />
object, the object appears larger because the lens bends<br />
the rays of light inward. The eye naturally traces the<br />
rays of light back toward the object in straight lines.<br />
It sees a “virtual” image, which is larger than the<br />
original image. The degree of magnification depends<br />
on the angles formed by the curvature of the lens.<br />
Plane mirror<br />
Incoming light<br />
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