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In this chapter you will discover…In this chapter you will discover…
 the connection between visible light, radio waves, Xthe connection between visible light, radio waves, X
rays and other types of electromagnetic radiationrays and other types of electromagnetic radiation
 the debate in past centuries over what light is and howthe debate in past centuries over what light is and how
Einstein resolved this questionEinstein resolved this question
 how telescopes collect and focus lighthow telescopes collect and focus light
 why different types of telescopes are used for differentwhy different types of telescopes are used for different
types of researchtypes of research
 the limitations of telescopes, especially those that usethe limitations of telescopes, especially those that use
lenses to collect lightlenses to collect light
 what the new generations of land-based and space-what the new generations of land-based and space-
based high-technology telescopes being developed canbased high-technology telescopes being developed can
dodo
 how astronomers use the entire spectrum ofhow astronomers use the entire spectrum of
electromagnetic radiation to observe the stars and otherelectromagnetic radiation to observe the stars and other
astronomical objects and eventsastronomical objects and events
When a beam of white light passes through a glass
prism, the light is separated or refracted into a
rainbow-colored band called a spectrum. The
numbers on the right side of the spectrum indicate
wavelengths in nanometers (1 nm = 10–9
m).
Prisms and a Spectrum
This drawing of Newton’s experiment illustrates that glass
does not add to the color of light, only changes its direction.
Because color is not added, this experiment shows that color
is an intrinsic property of light.
Prisms and a Spectrum
Wave Travel
(a) Water waves passing through two slits in a ripple tank create interference
patterns. The water waves interfere with each other, creating constructive
interference (crests) and destructive interference (troughs) throughout the right
side of the tank and on the far right wall.
(b) Electromagnetic radiation also travels as waves. Thomas Young’s
interference experiment shows that light of a single color passing
through a barrier with two slits behaves as waves that create alternating
light and dark patterns on a screen.
Wave Travel
Electromagnetic Radiation
 In 1860, James Clerk Maxwell combined and unified the currentIn 1860, James Clerk Maxwell combined and unified the current
theories of electricity and magnetism and showed that electrictheories of electricity and magnetism and showed that electric
and magnetic fields should travel through space together in theand magnetic fields should travel through space together in the
form of electromagnetic waves.form of electromagnetic waves.
 All forms of electromagnetic radiation (radio waves, infraredAll forms of electromagnetic radiation (radio waves, infrared
radiation, visible light, ultraviolet radiation, X rays, and gammaradiation, visible light, ultraviolet radiation, X rays, and gamma
rays) consist of electric and magnetic fields oscillatingrays) consist of electric and magnetic fields oscillating
perpendicular to each other and to the direction they move.perpendicular to each other and to the direction they move.
 The distance between two successive crests, denoted byThe distance between two successive crests, denoted by λλ, is, is
called the wavelength of the light.called the wavelength of the light.
The Nature of LightThe Nature of Light
 Despite the name electromagnetic radiation, neither visibleDespite the name electromagnetic radiation, neither visible
light nor any other type of electromagnetic radiation islight nor any other type of electromagnetic radiation is
electrically charged.electrically charged.
 Refraction or bending of light is dependent on wavelength.Refraction or bending of light is dependent on wavelength.
The shorter the wavelength, the more light is refracted.The shorter the wavelength, the more light is refracted.
 The constant speed of light in a vacuum (a region thatThe constant speed of light in a vacuum (a region that
contains no matter) is 3.0 x 10contains no matter) is 3.0 x 1055
km/s (1.86 x 10km/s (1.86 x 1055
mi/s).mi/s).
 Einstein proposed that light travels as waves enclosed inEinstein proposed that light travels as waves enclosed in
discrete packets called photons, and that photons withdiscrete packets called photons, and that photons with
different wavelengths have different amounts of energy.different wavelengths have different amounts of energy.
Ole Rømer used two eclipses of one of Jupiter’s moons to first
show that light does not travel infinitely fast and to measure its
speed. One can also use Maxwell’s equations to calculate the
speed of light (c = 3.0 x 105
km/s = 1.86 x 105
mi/s).
Evidence that Light Travels at a Finite Speed
This photograph shows the visible
colors separated by a prism. The
two thermometers in the region
illuminated by visible light have
temperatures less than the
thermometer to the right of red.
Therefore, there must be more
radiation energizing (i.e., heating)
the warmest thermometer. This
energy is what we call infrared
radiation—invisible to the human
eye, but detectable as heat.
Experimental Evidence for Infrared Radiation
There are a wide range of wavelengths
of electromagnetic waves which are
plotted on the electromagnetic
spectrum. We classify these waves
depending on their source, use, or
interactions with other matter.
Only a very small range of
wavelengths, 400nm to 700nm, is
visible to humans. (Since these
wavelengths are small, we describe
them in terms of nanometers (10–9
m)
or angstroms (Å; 10–10
m).
Other wavelengths are classified as
gamma rays, X rays, ultraviolet
radiation, infrared radiation,
microwaves, or radio waves.
The Electromagnetic Spectrum
The transparency of a material depends on the wavelength of light.
Earth’s atmosphere is relatively transparent to visible light and radio
waves, which are referred to as “windows” through which we can view
space from a ground-based telescope.
“Windows” Through the Atmosphere
This replica of Newton’s reflecting telescope was built in
1672. This reflecting telescope has a spherical primary
mirror 3 cm (1.3 in.) in diameter. Its magnification was
40x.
Replica of Newton’s Reflecting Telescope
The angle at which a
beam of light strikes
a mirror (the angle of
incidence, i ) is
always equal to the
angle at which the
beam is reflected
from the mirror (the
angle of reflection, r).
Reflection
The large mirror used to
gather and focus the light
in a reflecting telescope is
called the primary mirror.
The surface of the mirror
used is bent into a curve.
Parallel light rays from
distant objects converge
to a focal point.
The distance between the
mirror and its focal point
is called the focal length.
Reflection
A Newtonian telescope uses
a flat secondary mirror to
redirect the focused image to
the side of the telescope for
viewing. The image is
viewed through a small focal
length lens called an
eyepiece. The dashed line
shows where the focal point
of this primary mirror would
be if the secondary mirror
were not in the way.
Reflection
Even though light rays from stars
spread out in all directions, they
must travel over huge interstellar
distances to reach Earth.
Therefore, the rays that enter our
telescopes are essentially traveling
in the same direction and thus are
considered parallel.
If the object we are examining is
an extended object, such as the
Moon, then the light rays converge
in a focal plane rather than a single
point.
Parallel Light Rays from Distant Objects
Four of the most common optical designs for reflecting telescopes: (a)
Newtonian focus (popular among amateur astronomers) and the three
major designs used by researchers—(b) Cassegrain focus, (c) Nasmyth
focus or coudé focus, and (d) prime focus.
Reflecting Telescopes
Secondary Mirror of a Reflecting Telescope Does
Not Create a Hole in the Image
Because the light rays from distant
objects are parallel, light from the entire
object (in this case, the crescent Moon)
reflects off all parts of the primary
mirror. Therefore, every part of the
object sends photons to the eyepiece.
This figure shows the reconstruction of
the entire crescent Moon from light
passing through just part of this
telescope. The same drawing applies
everywhere on the primary mirror that is
not blocked by the secondary mirror.
Because a large primary mirror collects more starlight than does a smaller one, a larger
telescope produces a brighter image than a smaller one, all other things being equal.
The same principle applies to telescopes that collect light using just lenses. The two
photographs of the Andromeda Galaxy were taken through telescopes with different
diameters and were exposed for equal lengths of time at equal magnification.
Light-Gathering Power
Resolution (Clarity of Images)
The larger the diameter of a telescope’s primary mirror, the finer the detail the
telescope can resolve. These two images of the Andromeda Galaxy, taken
through telescopes with different diameters, show this effect. (a) A lower-
resolution image taken through a smaller telescope. In this photograph most
individual stars blur together to make the galaxies look like fuzzy blobs. (b) The
same field of view through a larger-diameter telescope. Many more individual
stars and interstellar gas clouds are visible here than in (a). Increasing the
exposure time of the smaller-diameter telescope (a) will only brighten the
image, not improve the resolution.
The same telescope can magnify by different amounts, depending on
the focal length of the eyepiece. (a) A low-magnification image of the
Moon. (b) An image of the Moon taken with magnification four times
greater than image (a). Note in this case that the increased
magnification leads to increased resolution (i.e., more detail can be seen
in the larger image).
Magnification
Telescopes Brighten, Resolve, and MagnifyTelescopes Brighten, Resolve, and Magnify
 A mirror with twice the diameter of another mirror willA mirror with twice the diameter of another mirror will
collect four times as much light as the smaller one in thecollect four times as much light as the smaller one in the
same amount of time.same amount of time.
 A telescope with a primary mirror twice the diameter ofA telescope with a primary mirror twice the diameter of
another telescope’s primary mirror will be able to seeanother telescope’s primary mirror will be able to see
twice as much detail as the smaller telescope.twice as much detail as the smaller telescope.
 A telescope with a primary mirror twice the diameter ofA telescope with a primary mirror twice the diameter of
another telescope’s primary mirror will have twice theanother telescope’s primary mirror will have twice the
magnification of the smaller telescope.magnification of the smaller telescope.
(a) Refraction is the change in direction of a light ray when it passes into or out of a
transparent medium such as glass. A light ray that enters a denser medium, such as
moving from air into water or glass, is bent or refracted to an angle more perpendicular
to the surface than the angle at which it was originally traveling. If the glass is flat, then
the light leaving it is refracted back to the direction it had before entering the glass.
There is no overall change in the direction in which the light travels. (b) If the glass is in
the shape of a suitable convex lens, parallel light rays converge to a focus at the focal
point. As with parabolic mirrors, the distance from the lens to the focal point is called the
focal length of the lens
Refraction Through Uniform and Variable Thickness Glasses
Refraction of Straw Through Two Mediums
(c) The straw as seen through the side of the liquid is magnified and offset from the
straw above the liquid because the liquid is given a curved shape by the side of the
glass. The straw, as seen through the top of the liquid, is refracted but does not appear
magnified because the surface of the water is flat and the beaker has uniform thickness.
Light from objects
larger than points in
the sky does not all
converge to the focal
point of a lens. Rather,
an image of the object
is created at the focal
length in what is called
the focal plane.
Extended Objects Create a Focal Plane
A refracting telescope consists of a large, long-focal-length
objective lens that collects and focuses light rays and a small,
short-focal-length eyepiece lens that restraightens the light rays.
The lenses work together to brighten, resolve, and magnify the
image formed at the focal plane of the objective lens.
Essentials of a Refracting Telescope
This giant refracting telescope,
built in the late 1800s, is
housed at Yerkes Observatory
near Chicago. The objective
lens is 102 cm (40 in.) in
diameter, and the telescope
tube is 19⅓ m (63½ ft.) long.
The Largest Refracting Telescope
If both sides of a lens are spherical surfaces, as shown here, then light rays of
the same color passing through at different distances from the center of the
lens are refracted by different amounts. Therefore, spherical lenses have
different focal lengths for these different light rays and so they give blurry
images.
The Geometry of a Spherical Lens
Chromatic Aberration
(a) Light of different wavelengths is refracted by different amounts when
passing through a medium such as glass. Therefore, single lenses such as this
one have different focal lengths for light of different colors passing through
them. (b) Image showing chromatic aberration. Note the different colors on the
edges of the petals caused by light passing through a lens.
Achromatic Lens
(a) By using two differently shaped lenses (often of different types of glass),
light of different wavelengths can be brought into focus at the same focal
length. Such achromatic lenses are used in cameras and many telescopes. (b)
Same object as in Figure 3-21b imaged through an achromatic lens. Note that
the colors on the edges of the petals seen in Figure 3-21b do not occur here.
When a spherically
shaped mirror is used,
the light rays hitting far
from the center do not
converge at the same
point. One solution is to
instead grind the mirror
into a parabolic shape.
Another solution is to
use a correcting lens to
make all the light rays
converge at a single
point.
Spherical Aberration
Difficulties with Refracting TelescopesDifficulties with Refracting Telescopes
 A lens must be supported only around its edgesA lens must be supported only around its edges
to avoid blocking the light. The weight of a largeto avoid blocking the light. The weight of a large
lens can cause it to sag and thus distort thelens can cause it to sag and thus distort the
image. This distortion is not a problem withimage. This distortion is not a problem with
reflectors because the entire underside of thereflectors because the entire underside of the
mirror can be supported, as necessary.mirror can be supported, as necessary.
 Air bubbles in the glass cause unwantedAir bubbles in the glass cause unwanted
refractions and, hence, distorted images.refractions and, hence, distorted images.
 Glass does not allow all wavelengths to passGlass does not allow all wavelengths to pass
through it equally.through it equally.
(a) To make each 8.4-m primary
mirror for the Large Binocular
Telescope II on Mount Graham in
Arizona, 40,000 pounds of glass are
loaded into a rotating furnace and
heated to 1450 K (2150°F). This
image shows glass fragments
loaded into the cylindrical furnace.
(b) After melting, spinning, and
cooling, the mirror’s parabolic
surface is ready for final smoothing
and coating with a highly reflective
material.
Rotating Furnace for Making
Parabolic Telescope Mirrors
(a) New technology has created charge-coupled devices (CCDs) that gather
light more efficiently than photographic plates. (b) This image of the Rosette
Nebula, a region of star formation 5000 ly away in the constellation Monoceros
(the Unicorn), was taken with this CCD. It shows the incredible detail that can
be recorded by large telescopes and high-resolution CCDs.
Mosaic of Charge-Coupled Devices (CCDs)
These three views of the same part of the sky, each taken with the same 4-m
telescope, compare CCDs to photographic plates. (a) A negative print (black
stars and white sky) of a photographic image. (b) A negative CCD image.
Notice that many faint stars and galaxies that are invisible in the ordinary
photograph can be seen clearly in this CCD image. (c) This (positive) color
view was produced by combining a series of CCD images taken through
colored filters.
Photography versus CCD Images
The same star field photographed with (a) a ground-based
telescope, which is subject to poor seeing conditions that
result in stars twinkling, and (b) the Hubble Space
Telescope, which is free from the effects of twinkling.
Effects of Twinkling
Light Pollution
These two images of New York
City, as seen from under the
Brooklyn Bridge, show the
increase of light in the sky from
1955 to 2010. Compare the
skies just above the buildings.
This light prevents New Yorkers
from seeing dimmer stars that
are visible in darker locations.
Since 1972, light pollution, a
problem for many observatories
around the world, has been
partially controlled by local
ordinances passed by cities.
This photograph of the Hubble Space Telescope (HST) hovering above
the space shuttle’s cargo bay was taken in 1993, at completion of the
first servicing mission. HST has studied the heavens at infrared, visible
light, and ultraviolet wavelengths.
The Hubble Space Telescope (HST)
Using adaptive optics, which calculate the amount of twinkling of our
atmosphere and change the shape of the mirror accordingly, we can receive
better images from ground-based telescopes. (a) Image of Neptune from an
Earth-based telescope without adaptive optics. (b) Image of Neptune from the
same Earth-based telescope with adaptive optics. (c) Image of Neptune from
the Hubble Space Telescope, which does not incorporate adaptive optics
technology.
Images from Earth and Space
The 10-m Keck telescopes are
located on the dormant (and
hopefully extinct) Mauna Kea
volcano in Hawaii. These huge
twin telescopes each consist of
36 hexagonal mirrors measuring
1.8 m (5.9 ft.) across. Each Keck
telescope has the light-gathering,
resolving, and magnifying ability
of a single mirror 10 m in
diameter. Inset: View down the
Keck I telescope. The hexagonal
apparatus near the top of the
photograph shows the housing for
the 1.4-m secondary mirror.
Keck Telescopes
(a) This is an ordinary optical photograph of the constellation Orion. (b) This is
an ultraviolet image of Orion. (c) A false-color view from the Infrared
Astronomical Satellite of the entire Orion asterism. Different colors indicate
different intensities of infrared radiation. Clearly, different wavelengths provide
different information about various objects in space.
Orion as Seen in Visible, Ultraviolet, and Infrared Wavelengths
Recall that the secondary mirror or
prime focus on most telescopes blocks
incoming light or other radiation. This
new radio telescope at the National
Radio Astronomy Observatory in
Green Bank, West Virginia, has its
prime focus hardware located off-
center from the telescope’s 100m x
110m oval reflector. By using this new
design, there is no such loss of signal.
Such configurations are also common
on microwave dishes used to receive
satellite transmissions for home
televisions.
National Radio Astronomy
Observatory, Green Bank, WV
A Radio Telescope
The 27 radio telescopes of the Very Large Array (VLA) system are arranged along the
arms of a Y in central New Mexico. Besides being able to change the angles at which
they observe the sky, these telescopes can be moved by train cars so that the array can
detect either wide areas of the sky (when the telescopes are close together, as in this
photograph) or small areas with higher resolution (when they are farther apart). The inset
shows the traditional secondary mirror assembly in the center of each of these antennas.
The Karl G. Jansky Very Large Array
VISIBLE LIGHT RADIO WAVES
The visible light picture was taken by a camera on board a
spacecraft as it approached Saturn. The view was produced by
sunlight scattered from the planet’s cloud tops and rings. The
radio image is a false-color picture, taken by the VLA, and shows
radio emission from Saturn at a wavelength of 2 cm.
Visible and Radio Views of Saturn
Infrared radiation can travel through
media that block visible light.
Kissing Is Hot
The infrared (heat) from this kissing couple
has been converted into visible light colors
so that we can interpret the invisible
radiation. The hottest regions are white,
with successively cooler areas shown in
yellow, orange, red, green, sky blue, dark
blue, and violet.
(a) The mirror assembly for the Spitzer Space Telescope, showing the 85-cm objective
mirror. (b) Launched in 2003, this Great Observatory is taking images and spectra of
planets, comets, gas, and dust around other stars and in interstellar space, galaxies, and
the large-scale distribution of matter in the universe. Inset: An infrared image of a region
of star formation invisible to optical telescopes.
Spitzer Space Telescope
Views of the Milky Way’s Central Regions
(a) An optical image in the direction of Sagittarius, toward the Milky Way’s
center, showing many nearby stars. The dark regions are interstellar gas and
dust clouds that prevent visible light from beyond them from reaching us. (b) An
infrared image of the same area of the sky, showing many more distant stars
whose infrared radiation passes through the clouds and is collected by our
telescopes.
(a) The McMath-Pierce Solar Telescope at Kitt Peak Observatory near Tucson, Arizona
(the inverted V-shaped structure), takes visible-light photographs of the Sun, such as the
one shown in the inset. (b) This X-ray telescope was carried aloft in 1994 by the space
shuttle. The inset shows an X-ray image of the Sun. Comparing the images in the two
insets reveals how important observing nonvisible radiation from astronomical
phenomena is to furthering our understanding of how the universe operates.
Nonvisible and Visible Radiation
(a) X-rays penetrate objects
they strike head-on. In order to
be focused, X-rays have to be
gently nudged by skimming off
cylindrical “mirrors.” (b) The
shapes of the mirrors optimize
the focus. (c) The diagram
shows how X-rays are focused
in the Chandra X-ray Telescope.
Grazing Incidence X-ray Telescopes
Survey of the Universe in Various Parts of the Electromagnetic Spectrum
(a) Radio Waves
(c) Visible Light(b) Infrared Radiation
(d) X rays (e) Gamma rays
Summary of Key IdeasSummary of Key Ideas
The Nature Of Light
 Photons, units of vibrating electric and magnetic fields, allPhotons, units of vibrating electric and magnetic fields, all
carry energy through space at the same speed, the speed ofcarry energy through space at the same speed, the speed of
light (300,000 km/s in a vacuum, slower in any medium).light (300,000 km/s in a vacuum, slower in any medium).
 Radio waves, microwaves, infrared radiation, visible light,Radio waves, microwaves, infrared radiation, visible light,
ultraviolet radiation, X rays, and gamma rays are the forms ofultraviolet radiation, X rays, and gamma rays are the forms of
electromagnetic radiation. They travel as photons, sometimeselectromagnetic radiation. They travel as photons, sometimes
behaving as particles, sometimes as waves.behaving as particles, sometimes as waves.
 Visible light occupies only a small portion of theVisible light occupies only a small portion of the
electromagnetic spectrum.electromagnetic spectrum.
 The wavelength of a visible-light photon is associated with itsThe wavelength of a visible-light photon is associated with its
color. Wavelengths of visible light range from about 400 nmcolor. Wavelengths of visible light range from about 400 nm
for violet light to 700 nm for red light.for violet light to 700 nm for red light.
 Infrared radiation, microwaves, and radio waves haveInfrared radiation, microwaves, and radio waves have
wavelengths longer than those of visible light. Ultravioletwavelengths longer than those of visible light. Ultraviolet
radiation, X rays, and gamma rays have wavelengths that areradiation, X rays, and gamma rays have wavelengths that are
shorter.shorter.
Optics and Telescopes
 A telescope’s most important function is to gather asA telescope’s most important function is to gather as
much light as possible. When possible, it also resolvesmuch light as possible. When possible, it also resolves
(reveals details) and magnifies an object.(reveals details) and magnifies an object.
 Reflecting telescopes, or reflectors, produce images byReflecting telescopes, or reflectors, produce images by
reflecting light rays from concave mirrors to a focal pointreflecting light rays from concave mirrors to a focal point
or focal plane.or focal plane.
 Refracting telescopes, or refractors, produce images byRefracting telescopes, or refractors, produce images by
bending light rays as they pass through glass lenses.bending light rays as they pass through glass lenses.
Glass impurity, opacity to certain wavelengths, andGlass impurity, opacity to certain wavelengths, and
structural difficulties make it inadvisable to buildstructural difficulties make it inadvisable to build
extremely large refractors. Reflectors are not subject toextremely large refractors. Reflectors are not subject to
the problems that limit the usefulness of refractors.the problems that limit the usefulness of refractors.
 Earth-based telescopes are being built with active opticsEarth-based telescopes are being built with active optics
and adaptive optics. These advanced technologies yieldand adaptive optics. These advanced technologies yield
resolving power comparable to the Hubble Spaceresolving power comparable to the Hubble Space
Telescope.Telescope.
Nonoptical Astronomy
 Radio telescopes have large, reflecting antennasRadio telescopes have large, reflecting antennas
(dishes) that are used to focus radio waves.(dishes) that are used to focus radio waves.
 Very sharp radio images are produced with arrays ofVery sharp radio images are produced with arrays of
radio telescopes linked together in a technique calledradio telescopes linked together in a technique called
interferometry.interferometry.
 Earth’s atmosphere is fairly transparent to most visibleEarth’s atmosphere is fairly transparent to most visible
light and radio waves, along with some infrared andlight and radio waves, along with some infrared and
ultraviolet radiation arriving from space, but it absorbsultraviolet radiation arriving from space, but it absorbs
much of the electromagnetic radiation at othermuch of the electromagnetic radiation at other
wavelengths.wavelengths.
Nonoptical Astronomy
 For observations at other wavelengths, astronomersFor observations at other wavelengths, astronomers
mostly depend on telescopes carried above themostly depend on telescopes carried above the
atmosphere by rockets. Satellite-based observatoriesatmosphere by rockets. Satellite-based observatories
are giving us a wealth of new information about theare giving us a wealth of new information about the
universe and permitting coordinated observation of theuniverse and permitting coordinated observation of the
sky at all wavelengths.sky at all wavelengths.
 Charge-coupled devices (CCDs) record images on manyCharge-coupled devices (CCDs) record images on many
telescopes used between infrared and X-raytelescopes used between infrared and X-ray
wavelengths.wavelengths.
Key TermsKey Terms
active optics
adaptive optics
angular resolution
(resolution)
Cassegrain focus
charge-coupled device
chromatic aberration
coudé focus
electromagnetic radiation
electromagnetic spectrum
eyepiece lens
focal length
focal plane
focal point
frequency
gamma ray
infrared radiation
interferometry
light-gathering power
magnification
Newtonian reflector
objective lens
photon
pixel
primary mirror
prime focus
radio telescope
radio wave
reflecting telescope
(reflector)
reflection
refracting telescope
refraction
refractor
Schmidt corrector plate
secondary mirror
seeing disk
spectrum (plural
spectra)
spherical aberration
twinkling
ultraviolet (UV)
radiation
very-long-baseline
interferometry (VLBI)
wavelength
X-ray

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Dtu10e lecture ppt_ch03

  • 1.
  • 2. In this chapter you will discover…In this chapter you will discover…  the connection between visible light, radio waves, Xthe connection between visible light, radio waves, X rays and other types of electromagnetic radiationrays and other types of electromagnetic radiation  the debate in past centuries over what light is and howthe debate in past centuries over what light is and how Einstein resolved this questionEinstein resolved this question  how telescopes collect and focus lighthow telescopes collect and focus light  why different types of telescopes are used for differentwhy different types of telescopes are used for different types of researchtypes of research  the limitations of telescopes, especially those that usethe limitations of telescopes, especially those that use lenses to collect lightlenses to collect light  what the new generations of land-based and space-what the new generations of land-based and space- based high-technology telescopes being developed canbased high-technology telescopes being developed can dodo  how astronomers use the entire spectrum ofhow astronomers use the entire spectrum of electromagnetic radiation to observe the stars and otherelectromagnetic radiation to observe the stars and other astronomical objects and eventsastronomical objects and events
  • 3. When a beam of white light passes through a glass prism, the light is separated or refracted into a rainbow-colored band called a spectrum. The numbers on the right side of the spectrum indicate wavelengths in nanometers (1 nm = 10–9 m). Prisms and a Spectrum
  • 4. This drawing of Newton’s experiment illustrates that glass does not add to the color of light, only changes its direction. Because color is not added, this experiment shows that color is an intrinsic property of light. Prisms and a Spectrum
  • 5. Wave Travel (a) Water waves passing through two slits in a ripple tank create interference patterns. The water waves interfere with each other, creating constructive interference (crests) and destructive interference (troughs) throughout the right side of the tank and on the far right wall.
  • 6. (b) Electromagnetic radiation also travels as waves. Thomas Young’s interference experiment shows that light of a single color passing through a barrier with two slits behaves as waves that create alternating light and dark patterns on a screen. Wave Travel
  • 7. Electromagnetic Radiation  In 1860, James Clerk Maxwell combined and unified the currentIn 1860, James Clerk Maxwell combined and unified the current theories of electricity and magnetism and showed that electrictheories of electricity and magnetism and showed that electric and magnetic fields should travel through space together in theand magnetic fields should travel through space together in the form of electromagnetic waves.form of electromagnetic waves.  All forms of electromagnetic radiation (radio waves, infraredAll forms of electromagnetic radiation (radio waves, infrared radiation, visible light, ultraviolet radiation, X rays, and gammaradiation, visible light, ultraviolet radiation, X rays, and gamma rays) consist of electric and magnetic fields oscillatingrays) consist of electric and magnetic fields oscillating perpendicular to each other and to the direction they move.perpendicular to each other and to the direction they move.  The distance between two successive crests, denoted byThe distance between two successive crests, denoted by λλ, is, is called the wavelength of the light.called the wavelength of the light.
  • 8. The Nature of LightThe Nature of Light  Despite the name electromagnetic radiation, neither visibleDespite the name electromagnetic radiation, neither visible light nor any other type of electromagnetic radiation islight nor any other type of electromagnetic radiation is electrically charged.electrically charged.  Refraction or bending of light is dependent on wavelength.Refraction or bending of light is dependent on wavelength. The shorter the wavelength, the more light is refracted.The shorter the wavelength, the more light is refracted.  The constant speed of light in a vacuum (a region thatThe constant speed of light in a vacuum (a region that contains no matter) is 3.0 x 10contains no matter) is 3.0 x 1055 km/s (1.86 x 10km/s (1.86 x 1055 mi/s).mi/s).  Einstein proposed that light travels as waves enclosed inEinstein proposed that light travels as waves enclosed in discrete packets called photons, and that photons withdiscrete packets called photons, and that photons with different wavelengths have different amounts of energy.different wavelengths have different amounts of energy.
  • 9. Ole Rømer used two eclipses of one of Jupiter’s moons to first show that light does not travel infinitely fast and to measure its speed. One can also use Maxwell’s equations to calculate the speed of light (c = 3.0 x 105 km/s = 1.86 x 105 mi/s). Evidence that Light Travels at a Finite Speed
  • 10. This photograph shows the visible colors separated by a prism. The two thermometers in the region illuminated by visible light have temperatures less than the thermometer to the right of red. Therefore, there must be more radiation energizing (i.e., heating) the warmest thermometer. This energy is what we call infrared radiation—invisible to the human eye, but detectable as heat. Experimental Evidence for Infrared Radiation
  • 11. There are a wide range of wavelengths of electromagnetic waves which are plotted on the electromagnetic spectrum. We classify these waves depending on their source, use, or interactions with other matter. Only a very small range of wavelengths, 400nm to 700nm, is visible to humans. (Since these wavelengths are small, we describe them in terms of nanometers (10–9 m) or angstroms (Å; 10–10 m). Other wavelengths are classified as gamma rays, X rays, ultraviolet radiation, infrared radiation, microwaves, or radio waves. The Electromagnetic Spectrum
  • 12. The transparency of a material depends on the wavelength of light. Earth’s atmosphere is relatively transparent to visible light and radio waves, which are referred to as “windows” through which we can view space from a ground-based telescope. “Windows” Through the Atmosphere
  • 13. This replica of Newton’s reflecting telescope was built in 1672. This reflecting telescope has a spherical primary mirror 3 cm (1.3 in.) in diameter. Its magnification was 40x. Replica of Newton’s Reflecting Telescope
  • 14. The angle at which a beam of light strikes a mirror (the angle of incidence, i ) is always equal to the angle at which the beam is reflected from the mirror (the angle of reflection, r). Reflection
  • 15. The large mirror used to gather and focus the light in a reflecting telescope is called the primary mirror. The surface of the mirror used is bent into a curve. Parallel light rays from distant objects converge to a focal point. The distance between the mirror and its focal point is called the focal length. Reflection
  • 16. A Newtonian telescope uses a flat secondary mirror to redirect the focused image to the side of the telescope for viewing. The image is viewed through a small focal length lens called an eyepiece. The dashed line shows where the focal point of this primary mirror would be if the secondary mirror were not in the way. Reflection
  • 17. Even though light rays from stars spread out in all directions, they must travel over huge interstellar distances to reach Earth. Therefore, the rays that enter our telescopes are essentially traveling in the same direction and thus are considered parallel. If the object we are examining is an extended object, such as the Moon, then the light rays converge in a focal plane rather than a single point. Parallel Light Rays from Distant Objects
  • 18. Four of the most common optical designs for reflecting telescopes: (a) Newtonian focus (popular among amateur astronomers) and the three major designs used by researchers—(b) Cassegrain focus, (c) Nasmyth focus or coudé focus, and (d) prime focus. Reflecting Telescopes
  • 19. Secondary Mirror of a Reflecting Telescope Does Not Create a Hole in the Image Because the light rays from distant objects are parallel, light from the entire object (in this case, the crescent Moon) reflects off all parts of the primary mirror. Therefore, every part of the object sends photons to the eyepiece. This figure shows the reconstruction of the entire crescent Moon from light passing through just part of this telescope. The same drawing applies everywhere on the primary mirror that is not blocked by the secondary mirror.
  • 20. Because a large primary mirror collects more starlight than does a smaller one, a larger telescope produces a brighter image than a smaller one, all other things being equal. The same principle applies to telescopes that collect light using just lenses. The two photographs of the Andromeda Galaxy were taken through telescopes with different diameters and were exposed for equal lengths of time at equal magnification. Light-Gathering Power
  • 21. Resolution (Clarity of Images) The larger the diameter of a telescope’s primary mirror, the finer the detail the telescope can resolve. These two images of the Andromeda Galaxy, taken through telescopes with different diameters, show this effect. (a) A lower- resolution image taken through a smaller telescope. In this photograph most individual stars blur together to make the galaxies look like fuzzy blobs. (b) The same field of view through a larger-diameter telescope. Many more individual stars and interstellar gas clouds are visible here than in (a). Increasing the exposure time of the smaller-diameter telescope (a) will only brighten the image, not improve the resolution.
  • 22. The same telescope can magnify by different amounts, depending on the focal length of the eyepiece. (a) A low-magnification image of the Moon. (b) An image of the Moon taken with magnification four times greater than image (a). Note in this case that the increased magnification leads to increased resolution (i.e., more detail can be seen in the larger image). Magnification
  • 23. Telescopes Brighten, Resolve, and MagnifyTelescopes Brighten, Resolve, and Magnify  A mirror with twice the diameter of another mirror willA mirror with twice the diameter of another mirror will collect four times as much light as the smaller one in thecollect four times as much light as the smaller one in the same amount of time.same amount of time.  A telescope with a primary mirror twice the diameter ofA telescope with a primary mirror twice the diameter of another telescope’s primary mirror will be able to seeanother telescope’s primary mirror will be able to see twice as much detail as the smaller telescope.twice as much detail as the smaller telescope.  A telescope with a primary mirror twice the diameter ofA telescope with a primary mirror twice the diameter of another telescope’s primary mirror will have twice theanother telescope’s primary mirror will have twice the magnification of the smaller telescope.magnification of the smaller telescope.
  • 24. (a) Refraction is the change in direction of a light ray when it passes into or out of a transparent medium such as glass. A light ray that enters a denser medium, such as moving from air into water or glass, is bent or refracted to an angle more perpendicular to the surface than the angle at which it was originally traveling. If the glass is flat, then the light leaving it is refracted back to the direction it had before entering the glass. There is no overall change in the direction in which the light travels. (b) If the glass is in the shape of a suitable convex lens, parallel light rays converge to a focus at the focal point. As with parabolic mirrors, the distance from the lens to the focal point is called the focal length of the lens Refraction Through Uniform and Variable Thickness Glasses
  • 25. Refraction of Straw Through Two Mediums (c) The straw as seen through the side of the liquid is magnified and offset from the straw above the liquid because the liquid is given a curved shape by the side of the glass. The straw, as seen through the top of the liquid, is refracted but does not appear magnified because the surface of the water is flat and the beaker has uniform thickness.
  • 26. Light from objects larger than points in the sky does not all converge to the focal point of a lens. Rather, an image of the object is created at the focal length in what is called the focal plane. Extended Objects Create a Focal Plane
  • 27. A refracting telescope consists of a large, long-focal-length objective lens that collects and focuses light rays and a small, short-focal-length eyepiece lens that restraightens the light rays. The lenses work together to brighten, resolve, and magnify the image formed at the focal plane of the objective lens. Essentials of a Refracting Telescope
  • 28. This giant refracting telescope, built in the late 1800s, is housed at Yerkes Observatory near Chicago. The objective lens is 102 cm (40 in.) in diameter, and the telescope tube is 19⅓ m (63½ ft.) long. The Largest Refracting Telescope
  • 29. If both sides of a lens are spherical surfaces, as shown here, then light rays of the same color passing through at different distances from the center of the lens are refracted by different amounts. Therefore, spherical lenses have different focal lengths for these different light rays and so they give blurry images. The Geometry of a Spherical Lens
  • 30. Chromatic Aberration (a) Light of different wavelengths is refracted by different amounts when passing through a medium such as glass. Therefore, single lenses such as this one have different focal lengths for light of different colors passing through them. (b) Image showing chromatic aberration. Note the different colors on the edges of the petals caused by light passing through a lens.
  • 31. Achromatic Lens (a) By using two differently shaped lenses (often of different types of glass), light of different wavelengths can be brought into focus at the same focal length. Such achromatic lenses are used in cameras and many telescopes. (b) Same object as in Figure 3-21b imaged through an achromatic lens. Note that the colors on the edges of the petals seen in Figure 3-21b do not occur here.
  • 32. When a spherically shaped mirror is used, the light rays hitting far from the center do not converge at the same point. One solution is to instead grind the mirror into a parabolic shape. Another solution is to use a correcting lens to make all the light rays converge at a single point. Spherical Aberration
  • 33. Difficulties with Refracting TelescopesDifficulties with Refracting Telescopes  A lens must be supported only around its edgesA lens must be supported only around its edges to avoid blocking the light. The weight of a largeto avoid blocking the light. The weight of a large lens can cause it to sag and thus distort thelens can cause it to sag and thus distort the image. This distortion is not a problem withimage. This distortion is not a problem with reflectors because the entire underside of thereflectors because the entire underside of the mirror can be supported, as necessary.mirror can be supported, as necessary.  Air bubbles in the glass cause unwantedAir bubbles in the glass cause unwanted refractions and, hence, distorted images.refractions and, hence, distorted images.  Glass does not allow all wavelengths to passGlass does not allow all wavelengths to pass through it equally.through it equally.
  • 34. (a) To make each 8.4-m primary mirror for the Large Binocular Telescope II on Mount Graham in Arizona, 40,000 pounds of glass are loaded into a rotating furnace and heated to 1450 K (2150°F). This image shows glass fragments loaded into the cylindrical furnace. (b) After melting, spinning, and cooling, the mirror’s parabolic surface is ready for final smoothing and coating with a highly reflective material. Rotating Furnace for Making Parabolic Telescope Mirrors
  • 35. (a) New technology has created charge-coupled devices (CCDs) that gather light more efficiently than photographic plates. (b) This image of the Rosette Nebula, a region of star formation 5000 ly away in the constellation Monoceros (the Unicorn), was taken with this CCD. It shows the incredible detail that can be recorded by large telescopes and high-resolution CCDs. Mosaic of Charge-Coupled Devices (CCDs)
  • 36. These three views of the same part of the sky, each taken with the same 4-m telescope, compare CCDs to photographic plates. (a) A negative print (black stars and white sky) of a photographic image. (b) A negative CCD image. Notice that many faint stars and galaxies that are invisible in the ordinary photograph can be seen clearly in this CCD image. (c) This (positive) color view was produced by combining a series of CCD images taken through colored filters. Photography versus CCD Images
  • 37. The same star field photographed with (a) a ground-based telescope, which is subject to poor seeing conditions that result in stars twinkling, and (b) the Hubble Space Telescope, which is free from the effects of twinkling. Effects of Twinkling
  • 38. Light Pollution These two images of New York City, as seen from under the Brooklyn Bridge, show the increase of light in the sky from 1955 to 2010. Compare the skies just above the buildings. This light prevents New Yorkers from seeing dimmer stars that are visible in darker locations. Since 1972, light pollution, a problem for many observatories around the world, has been partially controlled by local ordinances passed by cities.
  • 39. This photograph of the Hubble Space Telescope (HST) hovering above the space shuttle’s cargo bay was taken in 1993, at completion of the first servicing mission. HST has studied the heavens at infrared, visible light, and ultraviolet wavelengths. The Hubble Space Telescope (HST)
  • 40. Using adaptive optics, which calculate the amount of twinkling of our atmosphere and change the shape of the mirror accordingly, we can receive better images from ground-based telescopes. (a) Image of Neptune from an Earth-based telescope without adaptive optics. (b) Image of Neptune from the same Earth-based telescope with adaptive optics. (c) Image of Neptune from the Hubble Space Telescope, which does not incorporate adaptive optics technology. Images from Earth and Space
  • 41. The 10-m Keck telescopes are located on the dormant (and hopefully extinct) Mauna Kea volcano in Hawaii. These huge twin telescopes each consist of 36 hexagonal mirrors measuring 1.8 m (5.9 ft.) across. Each Keck telescope has the light-gathering, resolving, and magnifying ability of a single mirror 10 m in diameter. Inset: View down the Keck I telescope. The hexagonal apparatus near the top of the photograph shows the housing for the 1.4-m secondary mirror. Keck Telescopes
  • 42. (a) This is an ordinary optical photograph of the constellation Orion. (b) This is an ultraviolet image of Orion. (c) A false-color view from the Infrared Astronomical Satellite of the entire Orion asterism. Different colors indicate different intensities of infrared radiation. Clearly, different wavelengths provide different information about various objects in space. Orion as Seen in Visible, Ultraviolet, and Infrared Wavelengths
  • 43. Recall that the secondary mirror or prime focus on most telescopes blocks incoming light or other radiation. This new radio telescope at the National Radio Astronomy Observatory in Green Bank, West Virginia, has its prime focus hardware located off- center from the telescope’s 100m x 110m oval reflector. By using this new design, there is no such loss of signal. Such configurations are also common on microwave dishes used to receive satellite transmissions for home televisions. National Radio Astronomy Observatory, Green Bank, WV A Radio Telescope
  • 44. The 27 radio telescopes of the Very Large Array (VLA) system are arranged along the arms of a Y in central New Mexico. Besides being able to change the angles at which they observe the sky, these telescopes can be moved by train cars so that the array can detect either wide areas of the sky (when the telescopes are close together, as in this photograph) or small areas with higher resolution (when they are farther apart). The inset shows the traditional secondary mirror assembly in the center of each of these antennas. The Karl G. Jansky Very Large Array
  • 45. VISIBLE LIGHT RADIO WAVES The visible light picture was taken by a camera on board a spacecraft as it approached Saturn. The view was produced by sunlight scattered from the planet’s cloud tops and rings. The radio image is a false-color picture, taken by the VLA, and shows radio emission from Saturn at a wavelength of 2 cm. Visible and Radio Views of Saturn
  • 46. Infrared radiation can travel through media that block visible light. Kissing Is Hot The infrared (heat) from this kissing couple has been converted into visible light colors so that we can interpret the invisible radiation. The hottest regions are white, with successively cooler areas shown in yellow, orange, red, green, sky blue, dark blue, and violet.
  • 47. (a) The mirror assembly for the Spitzer Space Telescope, showing the 85-cm objective mirror. (b) Launched in 2003, this Great Observatory is taking images and spectra of planets, comets, gas, and dust around other stars and in interstellar space, galaxies, and the large-scale distribution of matter in the universe. Inset: An infrared image of a region of star formation invisible to optical telescopes. Spitzer Space Telescope
  • 48. Views of the Milky Way’s Central Regions (a) An optical image in the direction of Sagittarius, toward the Milky Way’s center, showing many nearby stars. The dark regions are interstellar gas and dust clouds that prevent visible light from beyond them from reaching us. (b) An infrared image of the same area of the sky, showing many more distant stars whose infrared radiation passes through the clouds and is collected by our telescopes.
  • 49. (a) The McMath-Pierce Solar Telescope at Kitt Peak Observatory near Tucson, Arizona (the inverted V-shaped structure), takes visible-light photographs of the Sun, such as the one shown in the inset. (b) This X-ray telescope was carried aloft in 1994 by the space shuttle. The inset shows an X-ray image of the Sun. Comparing the images in the two insets reveals how important observing nonvisible radiation from astronomical phenomena is to furthering our understanding of how the universe operates. Nonvisible and Visible Radiation
  • 50. (a) X-rays penetrate objects they strike head-on. In order to be focused, X-rays have to be gently nudged by skimming off cylindrical “mirrors.” (b) The shapes of the mirrors optimize the focus. (c) The diagram shows how X-rays are focused in the Chandra X-ray Telescope. Grazing Incidence X-ray Telescopes
  • 51. Survey of the Universe in Various Parts of the Electromagnetic Spectrum (a) Radio Waves (c) Visible Light(b) Infrared Radiation (d) X rays (e) Gamma rays
  • 52. Summary of Key IdeasSummary of Key Ideas
  • 53. The Nature Of Light  Photons, units of vibrating electric and magnetic fields, allPhotons, units of vibrating electric and magnetic fields, all carry energy through space at the same speed, the speed ofcarry energy through space at the same speed, the speed of light (300,000 km/s in a vacuum, slower in any medium).light (300,000 km/s in a vacuum, slower in any medium).  Radio waves, microwaves, infrared radiation, visible light,Radio waves, microwaves, infrared radiation, visible light, ultraviolet radiation, X rays, and gamma rays are the forms ofultraviolet radiation, X rays, and gamma rays are the forms of electromagnetic radiation. They travel as photons, sometimeselectromagnetic radiation. They travel as photons, sometimes behaving as particles, sometimes as waves.behaving as particles, sometimes as waves.  Visible light occupies only a small portion of theVisible light occupies only a small portion of the electromagnetic spectrum.electromagnetic spectrum.  The wavelength of a visible-light photon is associated with itsThe wavelength of a visible-light photon is associated with its color. Wavelengths of visible light range from about 400 nmcolor. Wavelengths of visible light range from about 400 nm for violet light to 700 nm for red light.for violet light to 700 nm for red light.  Infrared radiation, microwaves, and radio waves haveInfrared radiation, microwaves, and radio waves have wavelengths longer than those of visible light. Ultravioletwavelengths longer than those of visible light. Ultraviolet radiation, X rays, and gamma rays have wavelengths that areradiation, X rays, and gamma rays have wavelengths that are shorter.shorter.
  • 54. Optics and Telescopes  A telescope’s most important function is to gather asA telescope’s most important function is to gather as much light as possible. When possible, it also resolvesmuch light as possible. When possible, it also resolves (reveals details) and magnifies an object.(reveals details) and magnifies an object.  Reflecting telescopes, or reflectors, produce images byReflecting telescopes, or reflectors, produce images by reflecting light rays from concave mirrors to a focal pointreflecting light rays from concave mirrors to a focal point or focal plane.or focal plane.  Refracting telescopes, or refractors, produce images byRefracting telescopes, or refractors, produce images by bending light rays as they pass through glass lenses.bending light rays as they pass through glass lenses. Glass impurity, opacity to certain wavelengths, andGlass impurity, opacity to certain wavelengths, and structural difficulties make it inadvisable to buildstructural difficulties make it inadvisable to build extremely large refractors. Reflectors are not subject toextremely large refractors. Reflectors are not subject to the problems that limit the usefulness of refractors.the problems that limit the usefulness of refractors.  Earth-based telescopes are being built with active opticsEarth-based telescopes are being built with active optics and adaptive optics. These advanced technologies yieldand adaptive optics. These advanced technologies yield resolving power comparable to the Hubble Spaceresolving power comparable to the Hubble Space Telescope.Telescope.
  • 55. Nonoptical Astronomy  Radio telescopes have large, reflecting antennasRadio telescopes have large, reflecting antennas (dishes) that are used to focus radio waves.(dishes) that are used to focus radio waves.  Very sharp radio images are produced with arrays ofVery sharp radio images are produced with arrays of radio telescopes linked together in a technique calledradio telescopes linked together in a technique called interferometry.interferometry.  Earth’s atmosphere is fairly transparent to most visibleEarth’s atmosphere is fairly transparent to most visible light and radio waves, along with some infrared andlight and radio waves, along with some infrared and ultraviolet radiation arriving from space, but it absorbsultraviolet radiation arriving from space, but it absorbs much of the electromagnetic radiation at othermuch of the electromagnetic radiation at other wavelengths.wavelengths.
  • 56. Nonoptical Astronomy  For observations at other wavelengths, astronomersFor observations at other wavelengths, astronomers mostly depend on telescopes carried above themostly depend on telescopes carried above the atmosphere by rockets. Satellite-based observatoriesatmosphere by rockets. Satellite-based observatories are giving us a wealth of new information about theare giving us a wealth of new information about the universe and permitting coordinated observation of theuniverse and permitting coordinated observation of the sky at all wavelengths.sky at all wavelengths.  Charge-coupled devices (CCDs) record images on manyCharge-coupled devices (CCDs) record images on many telescopes used between infrared and X-raytelescopes used between infrared and X-ray wavelengths.wavelengths.
  • 57. Key TermsKey Terms active optics adaptive optics angular resolution (resolution) Cassegrain focus charge-coupled device chromatic aberration coudé focus electromagnetic radiation electromagnetic spectrum eyepiece lens focal length focal plane focal point frequency gamma ray infrared radiation interferometry light-gathering power magnification Newtonian reflector objective lens photon pixel primary mirror prime focus radio telescope radio wave reflecting telescope (reflector) reflection refracting telescope refraction refractor Schmidt corrector plate secondary mirror seeing disk spectrum (plural spectra) spherical aberration twinkling ultraviolet (UV) radiation very-long-baseline interferometry (VLBI) wavelength X-ray

Editor's Notes

  1. The buildings containing the Very Large Telescope optical telescopes at the Paranal Observatory, Atacama, Chile. (Babak Tafreshi/Science Source)
  2. FIGURE 3-1 Prisms and a Spectrum (a) When a beam of white light passes through a glass prism, the light is separated or refracted into a rainbow-colored band called a spectrum. The numbers on the right side of the spectrum indicate wavelengths in nanometers (1 nm = 10–9 m).
  3. FIGURE 3-1 Prisms and a Spectrum (b) This drawing of Newton’s experiment illustrates that glass does not add to the color of light, only changes its direction. Because color is not added, this experiment shows that color is an intrinsic property of light.
  4. FIGURE 3-2 Wave Travel (a) Water waves passing through two slits in a ripple tank create interference patterns. The water waves interfere with each other, creating constructive interference (crests) and destructive interference (troughs) throughout the right side of the tank and on the far right wall. (Adapted from University of Colorado, Center for Integrated Plasma Studies, Boulder, CO)
  5. FIGURE 3-2 Wave Travel (b) Electromagnetic radiation also travels as waves. Thomas Young’s interference experiment shows that light of a single color passing through a barrier with two slits behaves as waves that create alternating light and dark patterns on a screen. (Adapted from University of Colorado, Center for Integrated Plasma Studies, Boulder, CO)
  6. FIGURE 3-3 Electromagnetic Radiation All forms of electromagnetic radiation (radio waves, infrared radiation, visible light, ultraviolet radiation, X rays, and gamma rays) consist of electric and magnetic fields oscillating perpendicular to each other and to the direction they move. In empty space this radiation travels at a speed of 3 x 105 km/s. These fields are the mathematical description of the electric and magnetic effects. The distance between two successive crests, denoted by λ, is called the wavelength of the light.
  7. Information from sections 3-1, 3-2, & 3-3.
  8. FIGURE 3-4 Evidence that Light Travels at a Finite Speed The times of the eclipses of Jupiter’s moons as seen from Earth depend on the relative positions of Jupiter, Earth, and the Sun. Rømer correctly attributed the variations in these times to the variations in the time that it takes light from these events to reach Earth.
  9. FIGURE 3-5 Experimental Evidence for Infrared Radiation This photograph shows the visible colors separated by a prism. The two thermometers in the region illuminated by visible light have temperatures less than the thermometer to the right of red. Therefore, there must be more radiation energizing (i.e., heating) the warmest thermometer. This energy is what we call infrared radiation—invisible to the human eye, but detectable as heat. (NASA/JPL-Caltech)
  10. FIGURE 3-6 The Electromagnetic Spectrum The full array of all types of electromagnetic radiation is called the electromagnetic spectrum. It extends from the longest-wavelength radio waves to the shortest-wavelength gamma rays. Visible light forms only a tiny portion of the full electromagnetic spectrum. Note that 1 µm (micrometer) is 10–6 m, and 1 nm (nanometer) is 10–9 m. The insets show how we are now using all parts of the electromagnetic spectrum here on Earth. (From top: Will and Deni McIntyre/Science Source; Ted Kinsman/Science Source; Chris Martin-Bahr/Science Source; Bart Broek/E+/Getty Images; Michael Haegele/Corbis; iStockphoto/Thinkstock)
  11. FIGURE 3-7 “Windows” Through the Atmosphere Different types of electromagnetic radiation penetrate into Earth’s atmosphere in varying amounts. Visible light, radio waves, short-wavelength infrared, and long-wavelength ultraviolet reach all the way to Earth’s surface. The other types of radiation are absorbed or scattered by the gases in the air at different characteristic altitudes (indicated by heights of windows). Although the atmosphere does not have actual “windows,” astronomers use the term to characterize the passage of radiation through it.
  12. FIGURE 3-8 Replica of Newton’s Reflecting Telescope Built in 1672, this reflecting telescope has a spherical primary mirror 3 cm (1.3 in.) in diameter. Its magnification was 40x. (Royal Greenwich Observatory/Science Source)
  13. FIGURE 3-9 Reflection The angle at which a beam of light strikes a mirror (the angle of incidence, i ) is always equal to the angle at which the beam is reflected from the mirror (the angle of reflection, r).
  14. FIGURE 3-9 Reflection (b) A concave, parabolic mirror causes parallel light rays to converge and meet at the focal point. The distance between the mirror and focal point is the focal length.
  15. FIGURE 3-9 Reflection (c) A Newtonian telescope uses a flat mirror, called the secondary mirror, to send light toward the side of the telescope. The light rays are made parallel again by passing through a lens, called the eyepiece. The dashed line shows where the focal point of this primary mirror would be if the secondary mirror were not in the way.
  16. FIGURE 3-10 Parallel Light Rays from Distant Objects As light travels away from any object, the light rays, all moving in straight lines, separate. By the time light has traveled trillions of kilometers, only the light rays moving in virtually parallel tracks are still near each other.
  17. FIGURE 3-11 Reflecting Telescopes Four of the most common optical designs for reflecting telescopes: (a) Newtonian focus (popular among amateur astronomers) and the three major designs used by researchers—(b) Cassegrain focus, (c) Nasmyth focus or coudé focus, and (d) prime focus.
  18. FIGURE 3-12 Secondary Mirror of a Reflecting Telescope Does Not Create a Hole in the Image Because the light rays from distant objects are parallel, light from the entire object (in this case, the crescent Moon) reflects off all parts of the primary mirror. Therefore, every part of the object sends photons to the eyepiece. This figure shows the reconstruction of the entire crescent Moon from light passing through just part of this telescope. The same drawing applies everywhere on the primary mirror that is not blocked by the secondary mirror.
  19. FIGURE 3-13 Light-Gathering Power Because a large primary mirror collects more starlight than does a smaller one, a larger telescope produces a brighter image than a smaller one, all other things being equal. The same principle applies to telescopes that collect light using just lenses. The two photographs of the Andromeda Galaxy were taken through telescopes with different diameters and were exposed for equal lengths of time at equal magnification. (Royal Observatory, Edinburgh/Science Source)
  20. FIGURE 3-14 Resolution The larger the diameter of a telescope’s primary mirror, the finer the detail the telescope can resolve. These two images of the Andromeda Galaxy, taken through telescopes with different diameters, show this effect. (a) A lower-resolution image taken through a smaller telescope. In this photograph most individual stars blur together to make the galaxies look like fuzzy blobs. (b) The same field of view through a larger-diameter telescope. Many more individual stars and interstellar gas clouds are visible here than in (a). Increasing the exposure time of the smaller-diameter telescope (a) will only brighten the image, not improve the resolution. (Royal Observatory, Edinburgh/Science Source)
  21. FIGURE 3-15 Magnification The same telescope can magnify by different amounts, depending on the focal length of the eyepiece. (a) A low-magnification image of the Moon. (b) An image of the Moon taken with magnification four times greater than image (a). Note in this case that the increased magnification leads to increased resolution (i.e., more detail can be seen in the larger image). (iStockphoto/Thinkstock)
  22. Information from section 3-7.
  23. FIGURE 3-16 Refraction Through Uniform and Variable Thickness Glasses (a) Refraction is the change in direction of a light ray when it passes into or out of a transparent medium such as glass. A light ray that enters a denser medium, such as moving from air into water or glass, is bent or refracted to an angle more perpendicular to the surface than the angle at which it was originally traveling. If the glass is flat, then the light leaving it is refracted back to the direction it had before entering the glass. There is no overall change in the direction in which the light travels. (b) If the glass is in the shape of a suitable convex lens, parallel light rays converge to a focus at the focal point. As with parabolic mirrors, the distance from the lens to the focal point is called the focal length of the lens.
  24. FIGURE 3-16 Refraction of Straw Through Two Mediums (c) The straw as seen through the side of the liquid is magnified and offset from the straw above the liquid because the liquid is given a curved shape by the side of the glass. The straw, as seen through the top of the liquid, is refracted but does not appear magnified because the surface of the water is flat and the beaker has uniform thickness. (c: cheyennezj/Shutterstock)
  25. FIGURE 3-17 Extended Objects Create a Focal Plane Light from objects larger than points in the sky does not all converge to the focal point of a lens. Rather, an image of the object is created at the focal length in what is called the focal plane.
  26. FIGURE 3-18 Essentials of a Refracting Telescope A refracting telescope consists of a large, long-focal-length objective lens that collects and focuses light rays and a small, short-focal-length eyepiece lens that restraightens the light rays. The lenses work together to brighten, resolve, and magnify the image formed at the focal plane of the objective lens.
  27. FIGURE 3-19 The Largest Refracting Telescope This giant refracting telescope, built in the late 1800s, is housed at Yerkes Observatory near Chicago. The objective lens is 102 cm (40 in.) in diameter, and the telescope tube is 19⅓ m (63½ ft.) long. (top: Roger Ressmeyer/Corbis; bottom: Kyle Cudworth)
  28. FIGURE 3-20 The Geometry of a Spherical Lens If both sides of a lens are spherical surfaces, as shown here, then light rays of the same color passing through at different distances from the center of the lens are refracted by different amounts. Therefore, spherical lenses have different focal lengths for these different light rays and so they give blurry images.
  29. FIGURE 3-21 Chromatic Aberration (a) Light of different wavelengths is refracted by different amounts when passing through a medium such as glass. Therefore, single lenses such as this one have different focal lengths for light of different colors passing through them. (b) Image showing chromatic aberration. Note the different colors on the edges of the petals caused by light passing through a lens. (GYRO PHOTOGR APHY/amanaimagesRF/Getty Images)
  30. FIGURE 3-22 Achromatic Lens (a) By using two differently shaped lenses (often of different types of glass), light of different wavelengths can be brought into focus at the same focal length. Such achromatic lenses are used in cameras and many telescopes. (b) Same object as in Figure 3-21b imaged through an achromatic lens. Note that the colors on the edges of the petals seen in Figure 3-21b do not occur here. (GYRO PHOTOGRAPHY/amanaimagesRF/Getty Images)
  31. FIGURE 3-23 Spherical Aberration (a) Different parts of a spherically concave mirror reflect light to slightly different focal points. This effect, spherical aberration, causes image blurring. This problem can be overcome by (b) using a parabolic mirror or (c) using a Schmidt corrector plate (a specially curved lens) in front of the telescope.
  32. Information from section 3-8.
  33. FIGURE 3-24 Rotating Furnace for Making Parabolic Telescope Mirrors (a) To make each 8.4-m primary mirror for the Large Binocular Telescope II on Mount Graham in Arizona, 40,000 pounds of glass are loaded into a rotating furnace and heated to 1450 K (2150°F). This image shows glass fragments loaded into the cylindrical furnace. (b) After melting, spinning, and cooling, the mirror’s parabolic surface is ready for final smoothing and coating with a highly reflective material. (a: Roger Ressmeyer/Corbis; b: Joe McNally/Getty Images)
  34. FIGURE 3-25 Mosaic of Charge-Coupled Devices (CCDs) (a) These 40 CCDs combine to provide up to 378 million light-sensitive pixels that store images collected by the Canada-France-Hawaii Telescope on the dormant volcano Mauna Kea in Hawaii. Electronic circuits transfer the data to a waiting computer. (b) This image of the Rosette Nebula, a region of star formation 5000 ly away in the constellation Monoceros (the Unicorn), was taken with the CCD in (a). The image shows the incredible detail that can be recorded by large telescopes and high-resolution CCDs. (a: J. C. Cuillandre/Canada-France-Hawaii Telescope; b: CFHT/Science Source)
  35. FIGURE 3-26 Photography versus CCD Images These three views of the same part of the sky, each taken with the same 4-m telescope, compare CCDs to photographic plates. (a) A negative print (black stars and white sky) of a photographic image. (b) A negative CCD image. Notice that many faint stars and galaxies that are invisible in the ordinary photograph can be seen clearly in this CCD image. (c) This (positive) color view was produced by combining a series of CCD images taken through colored filters. (Patrick Seitzer, NOAO)
  36. FIGURE 3-27 Effects of Twinkling The same star field photographed with (a) a ground-based telescope, which is subject to poor seeing conditions that result in stars twinkling, and (b) the Hubble Space Telescope, which is free from the effects of twinkling. (NASA/ESA)
  37. FIGURE 3-28 Light Pollution These two images of New York City, as seen from under the Brooklyn Bridge, show the increase of light in the sky from 1955 to 2010. Compare the skies just above the buildings. This light prevents New Yorkers from seeing dimmer stars that are visible in darker locations. Since 1972, light pollution, a problem for many observatories around the world, has been partially controlled by local ordinances passed by cities. (top: D. Corson/ClassicStock/Corbis; bottom: Anhgemus Photography/Flickr/Getty Images)
  38. FIGURE 3-29 The Hubble Space Telescope (HST) This photograph of HST hovering above the space shuttle’s cargo bay was taken in 1993, at completion of the first servicing mission. HST has studied the heavens at infrared, visible light, and ultraviolet wavelengths. (NASA)
  39. FIGURE 3-30 Images from Earth and Space (a) Image of Neptune from an Earth-based telescope without adaptive optics. (b) Image of Neptune from the same Earth-based telescope with adaptive optics. (c) Image of Neptune from the Hubble Space Telescope, which does not incorporate adaptive optics technology. (a & b: Courtesy of Center for Adaptive Optics, University of California; c: NASA, L. Sromovksy, and P. Fry, University of Wisconsin-Madison)
  40. FIGURE 3-31 The 10-m Keck Telescopes Located on the dormant (and hopefully extinct) Mauna Kea volcano in Hawaii, these huge twin telescopes each consist of 36 hexagonal mirrors measuring 1.8 m (5.9 ft.) across. Each Keck telescope has the light-gathering, resolving, and magnifying ability of a single mirror 10 m in diameter. Inset: View down the Keck I telescope. The hexagonal apparatus near the top of the photograph shows the housing for the 1.4-m secondary mirror. (Enrico Sacchetti/Science Source; inset: Laurie Hatch Photography)
  41. FIGURE 3-32 Orion as Seen in Visible, Ultraviolet, and Infrared Wavelengths (a) An ordinary optical photograph of the constellation Orion. (b) An ultraviolet image of Orion. (c) A false-color view from the Infrared Astronomical Satellite of the entire Orion asterism. Different colors indicate different intensities of infrared radiation. Clearly, different wavelengths provide different information about various objects in space. (a: iStockphoto/Thinkstock; b: Johns Hopkins University Applied Physics Laboratory; c: NASA/JPL-Caltech)
  42. FIGURE 3-33 A Radio Telescope Recall that the secondary mirror or prime focus on most telescopes blocks incoming light or other radiation. This new radio telescope at the National Radio Astronomy Observatory in Green Bank, West Virginia, has its prime focus hardware located off-center from the telescope’s 100m x 110m oval reflector. By using this new design, there is no such loss of signal from the equipment covering part of the telescope, unlike the effects of secondary mirrors on optical telescopes. Such configurations are also common on microwave dishes used to receive satellite transmissions for home televisions. (NRAO/AUI/NSF)
  43. FIGURE 3-34 The Karl G. Jansky Very Large Array The 27 radio telescopes of the Jansky VLA system are arranged along the arms of a Y in central New Mexico. Besides being able to change the angles at which they observe the sky, astronomers can also move these telescopes by train cars so that the array can detect either wide areas of the sky (when they are close together, as in this photograph) or small areas with higher resolution (when they are farther apart). The inset shows the traditional secondary mirror assembly in the center of each of these antennas. (Jim Sugar/Corbis; inset: David Nunuk/Science Source)
  44. FIGURE 3-35 Visible and Radio Views of Saturn (a) This picture was taken by a camera on board a spacecraft as it approached Saturn. The view was produced by sunlight scattered from the planet’s cloud tops and rings. (b) This false-color picture, taken by the VLA (the predecessor of the Jansky VLA), shows radio emission from Saturn at a wavelength of 2 cm. (a: NASA; b: Image courtesy of NR AO/AUI/NSF)
  45. Kissing Is Hot The infrared (heat) from this kissing couple has been converted into visible light colors so that we can interpret the invisible radiation. The hottest regions are white, with successively cooler areas shown in yellow, orange, red, green, sky blue, dark blue, and violet. (David Montrose, M.D./Custom Medical Stock Photo) Infrared radiation can travel through media that block visible light. (NASA/JPL-Caltech)
  46. FIGURE 3-36 Spitzer Space Telescope (a) The mirror assembly for the Spitzer Space Telescope showing the 85 cm objective mirror. (b) Launched in 2003, this Great Observatory is taking images and spectra of planets, comets, gas and dust around other stars and in interstellar space, galaxies, and the large-scale distribution of matter in the universe. Inset: An infrared image of a region of star formation invisible to optical telescopes. (a: Balz/SIRTF Science Center; b: NASA/JPL-Caltech; inset: NASA/JPL)
  47. Figure 3-37 Views of the Milky Way’s Central Regions (a) An optical image in the direction of Sagittarius, toward the Milky Way’s center, showing many nearby stars. The dark regions are interstellar gas and dust clouds that prevent visible light from beyond them from reaching us. (b) An infrared image of the same area of the sky, showing many more distant stars whose infrared radiation passes through the clouds and is collected by our telescopes. (a: Dennis di Cicco/CORBIS; b: Science Source)
  48. Figure 3-38 Nonvisible and Visible Radiation (a) The McMath-Pierce Solar Telescope at Kitt Peak Observatory near Tucson, Arizona (the inverted V-shaped structure), takes visible-light photographs of the Sun, such as the one shown in the inset. (b) This X-ray telescope was carried aloft in 1994 by the space shuttle. The inset shows an X-ray image of the Sun. Comparing the images in the two insets reveals how important observing nonvisible radiation from astronomical phenomena is to furthering our understanding of how the universe operates. (a: NOAO/AURA/NSF; inset: NASA/SDO/HMI; b: NASA; inset: Solar X-ray image from the Yohkoh mission of ISAS, Japan; the X-ray telescope was prepared by the Lockheed-Martin Solar and Astrophysics Laboratory, the National Astronomical Observatory of Japan, and the University of Tokyo with the support of NASA and ISAS)
  49. FIGURE 3-39 Grazing Incidence X-ray Telescopes (a) X-rays penetrate objects they strike head-on. In order to be focused, X-rays have to be gently nudged by skimming off cylindrical “mirrors.” (b) The shapes of the mirrors optimize the focus. (c) The diagram shows how X-rays are focused in the Chandra X-ray Telescope. (a & b: NASA/JPL-Caltech; c: NASA/CXC/D. Berry & A. Hobart)
  50. FIGURE 3-40 Survey of the Universe in Various Parts of the Electromagnetic Spectrum By mapping the celestial sphere onto a flat surface (like making a map of Earth), astronomers can see the overall distribution of strong or nearby energy sources in space. The center of our Galaxy’s disk cuts these images horizontally in half. Because most of the emissions shown in these images fall in this region, we know that most of the strong sources of various electromagnetic radiation as seen from Earth (except X-rays) are in our Galaxy: (a) radio waves, (b) infrared radiation, (c) visible light, (d) X-rays, and (e) gamma rays. (GFSC/NASA)