The main purposes of a telescope used for astronomy
are:
(a) to gather as much light as possible – this is done by using a large aperture lens
or mirror. The amount of light gathered depends on the AREA of the lens – so a lens with an
aperture of 300 mm diameter gathers four times a much light as one with an aperture of 150
mm diameter.
(b) to resolve fine detail – this is also done by using a large aperture lens
or mirror. The larger the aperture the finer the detail that can be seen. (Usually called the
resolving power of the telescope.)
(c) to magnify the image of a distant object – this is
done by using a lens or mirror with a long focal length. The actual magnification of a
telescope can be worked out from the formula:
(a) the
lenses are made of glass and because the light has to go through them the glass must be
perfect – there must be no bubbles of air in the glass
(b) the lenses can only be
supported around their edges and this is where they are thinnest and weakest. The largest
telescope lens in the world is on of a metre in diameter at Yerkes Observatory in the
USA
(c) lenses suffer from colour distortion – this means that when white light passes
through the lens it is split into the colours of the spectrum. Because violet light refracts more
than red light it is brought to a focus closer to the lens than the red light – this makes the
image coloured and blurred. This effect is called chromatic
aberration.
However for small telescopes refractors are usually better than refractors because they can be made of high quality glass with no defects and the colour effects can be eliminated by using special lenses called chromatic lenses.
Telescopes are best placed in
observatories on the tops of mountains for the following reasons:
(a) they are above dust
and other types of atmospheric pollution
(b) they are above low cloud, mist and
fog
(c) they are far from light pollution of large centres of population
(d) the air is
thinner and so there is less atmospheric absorption
(e) there are fewer convection
currents in the air so that the image does not suffer so much from image shake
Of course
the Hubble Space telescope is in an even better position – there is no atmospheric
absorption at all in space.
These are usually of one of two
types:
(a) equatorial where one axis of the mounting is lined up with the axis of the earth.
This type of mounting has the enormous advantage that when you have sighted on a star
you only have to move the telescope about one axis in order to follow it across the
sky.
(b) altazimuth – here the axes are horizontal and vertical. These types of
mountings are used by many very large telescopes as they can be computer controlled to
move to follow the star, but the telescope must continually move on both axes – up or down
and across.
(a) the glass of the mirror
does not have to be perfect throughout – only to have a perfect surface
(b) the mirror can
be supported across the whole of its back
(c) they do not suffer from the colour defects of
chromatic aberration
For these reasons all the really large telescopes in the world today
are reflectors. The largest ones have mirrors up to 10m in diameter.
The Newtonian reflector has an eyepiece at
the side of the tube which makes observing comfortable.
The Cassegrain has an
eyepiece below the main mirror which means that much heavy detection equipment can be
fitted here.
The secondary mirrors in the telescope tubes do not affect the quality of
the image – the small amount of light that they interrupt is negligible compared with the total
amount received by the main mirror.
All mirrors used in astronomical telescopes are
silvered on the front surface, otherwise the light would pass through the glass and both
colour distortion and multiple images would result. The metal used is actually aluminium,
vaporised onto the surface of the glass in a vacuum. It does not reflect quite so well as silver
but is better over the complete range of wavelengths of visible light.
The curvature of
the mirrors is usually accurate to within one eighth of a wavelength of green light!
Radio
telescopes
Radio astronomy began in 1930 when Karl Jansky detected radio waves
coming from a source in the Milky Way in the region of the constellation Sagittarius. In the
1940's Grote Reber made detailed radio maps of the sky and also detected radio emissions
from the Sun. Radio telescopes operate at radio wavelengths which are considerably longer
than optical wavelengths. For example neutral hydrogen within our galaxy and others emits
at a wavelength of 21 cm and radio telescopes are designed to detect this.
This
longer operating wavelength has a number of implications for the radio telescope:
(a) at
21 cm the Earth's atmosphere absorbs a different proportion of the radiation
(b) radio
telescopes can be used in the daytime
(c) to get good resolving power a radio telescope
must be made much bigger than its optical counterpart. In fact to achieve the same resolving
power a radio telescope would have to be 50 000 times larger than its optical
counterpart.
(d) the surface of a radio telescope does not need to be so 'smooth' as that
of an optical mirror. Accuracies of ± 0.005 m are quite acceptable as against ± 0.000 000 1 m
for the optical mirror surface.