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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 />

23

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