Instruments 1. Basic Optics 1. Rays of Light 2. Waves of light 3. Basic Imaging Systems 4. A Basic Telescope 5. Aberrations 6. Mirrors 2. Some Real Instruments 1. Keplerian Optics 2. Astronomical seeing 3. Detectors 3. Other Wavelengths 1. Radio Telescopes 2. Orbiting Astronomical Observatory 3. Hubble 4. Other improvements 1. Adaptive Optics Basic Optics Rays of Light The pin-hole camera allows a small amount of light to pass through an opening. However, because the whole is small, very little light passes, which makes measurements difficult. If the hole's diameter is increased, then the image becomes blurred. Converging Lens By using a converging lens, we can allow more light to pass through the hole, which increases our 'photon count.' A consequence of using a lens however, is that now the focal length, , is fixed. Fig. 1 A pinhole will project an inverted image on a plane. Fig. 2 The image will be in focus everywhere. It's size changes based on the position of the focal plane. F PHY 454 - instruments - J. Hedberg - 2018 updated on 2018-09-27 Page 1
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Instruments1. Basic Optics
1. Rays of Light2. Waves of light3. Basic Imaging Systems4. A Basic Telescope5. Aberrations6. Mirrors
2. Some Real Instruments1. Keplerian Optics2. Astronomical seeing3. Detectors
3. Other Wavelengths1. Radio Telescopes2. Orbiting Astronomical Observatory3. Hubble
4. Other improvements1. Adaptive Optics
Basic Optics
Rays of LightThe pin-hole camera allows a smallamount of light to pass through anopening. However, because the wholeis small, very little light passes, whichmakes measurements difficult. If thehole's diameter is increased, then theimage becomes blurred.
Converging LensBy using a converging lens, we can allow more light to pass through the hole,which increases our 'photon count.' A consequence of using a lens however, isthat now the focal length, , is fixed.
Fig.1A pinhole will project an invertedimage on a plane.
Fig.2The image will be in focuseverywhere. It's size changes based onthe position of the focal plane.
F
PHY 454 - instruments - J. Hedberg - 2018
updated on 2018-09-27 Page 1
Images
Light from stars
Waves of lightCoherent, mono-chromatic light passing through a circular aperture will bediffracted.
Airy Disc
Fig.3
Fig.4Changing the position of thescreen will result in a blurry image.
θ θ
F
lens focal plane
stars
d
Fig.5Two stars separated by an angle in the sky, will create images
separated by a distance on thedetection screen.
θ
d
D
circularaperture
screen
light intensity
incident light
L
θ1
Fig.6
PHY 454 - instruments - J. Hedberg - 2018
updated on 2018-09-27 Page 2
There is a limitUnresolved: if the central maximum falls inside the location of the firstminimum.
Unresolved point sources
Rayleigh Criterion
Basic Imaging Systems
The eyeNature has made many different eyeballs. Most operate on the principles of lenses we’ve just looked at.
Fig.7
Fig.8Two point sources gettingcloser.
-2 -1 0 1 2
Fig.9
= 1.22θminλ
D
PHY 454 - instruments - J. Hedberg - 2018
updated on 2018-09-27 Page 3
focusing the eyeFocusing on objects: We cannot adjust the position of the lens with respect tothe retina. So, the muscles around the eye change the shape of the lens, whichthen changes its focal length.
A Basic Telescope
Magnification:
AberrationsLenses aren't perfect.
Chromatic Aberration
retina
lens
cornea
iris
aqueoushumor
optic nerve
Fig.10The human eye
Fig.11Focusing the eye
objectlens 1
(objective)
real image
Fig.12
objectlens 1 lens 2
(objective) (eyepiece)
virtual image
Fig.13
M = =f1
f2
fobjective
feyepiece
PHY 454 - instruments - J. Hedberg - 2018
updated on 2018-09-27 Page 4
Since different colors will refract atdifferent angles, the focal point will beslightly different for differentwavelengths. This leads to ChromaticAberration.
Spherical AberrationEarlier, our thin lens approximation ignored the fact that the thickness of thelens changed as a function of distance away from the central axis.
This leads to rays having slightly different focal points depending on wherethey are incident on the lens. The further the rays are away from the centralaxis, the worse the SphericalAberration effect is.
Fixing aberrationsFortunately, by using a multi lens setup, we can correct these aberrations. Forexample, to correct the chromatic aberration caused by a converging lens wecan insert a diverging lens after the converging lens to refocus the differentcolors back to the same point.
Mirrors
Some Real InstrumentsGalileo's Telescope
Fig.14Chromatic Aberrations Fig.15Different Colors with havedifferent focal points
Fig.25The Great Paris ExhibitionTelescope of 1900, with an objectivelens of 1.25 m (49 in) in diameter, wasthe largest refracting telescope everconstructed. It was built as thecenterpiece of the Paris UniversalExhibition of 1900. 200 ft long. Too bigto use.
By Unknown - Le panorama (Paris,1900)., Public Domain,https://commons.wikimedia.org/w/index.php?curid=20083299
eyepiece
parabolic mirror
parallel rays
flat mirror
Fig.26A reflecting Telescope
Fig.27A replica of the Newton -Wickins telescope, Newton's third
PHY 454 - instruments - J. Hedberg - 2018
updated on 2018-09-27 Page 7
Where should we put these telescopes?Early telescopes could be placed near where people lived, since there were not a lot of lights to get in the way. Now,we usually put telescope as far away from people as possible.
Astronomical seeing
As light passes through the atmosphere, small variations in air density, usuallycaused by temperature fluctuations will disturb the incoming waves. There isturbulent mixing of air throughout much of the atmosphere (but noteverywhere)
reflecting telescope that waspresented to the Royal Society in 1766after being restored by Thomas Heath.It is described as the better of theinstruments Newton built
By User:Solipsist (Andrew Dunn) -www.andrewdunnphoto.com, CC BY-SA 2.0,https://commons.wikimedia.org/w/index.php?curid=513483
DetectorsWe can classify most of the standard astronomical instruments as either imaging cameras or spectrometers. Eitherway, we need to collect photons. That used to be done with chemical film, but we use digital methods. They have amuch greater quantumefficiency, which means that it requires fewer photons to trigger a detection by a pixel.
Photographic Plate: 1%Human Eye: 10%CCD: 80-90%
Charge-coupled Device: CCD
Other Wavelengths
Fig.30Mountain in the atmosphere
Fig.31A CCD device
0.2 µm 500 nm 1µm 10µm 100µm 1mm 1 cm 1.0 m
microwaveThermal IRReflected IRVisibleUV
trans
mis
sion
0
100 %
Wavelength
Fig.32The transparency of the atmosphere
PHY 454 - instruments - J. Hedberg - 2018
updated on 2018-09-27 Page 9
Radio TelescopesWhat about for EM radiation with frequencies and wavelengths not in thevisible spectrum?
What if is really big?
When looking at 21 cm wavelengths, a 300 meter dish will have a diffraction limited resolution of what?
Arecibo
Orbiting Astronomical ObservatoryLet's put a telescope above the atmosphere. There, instruments will be able to reach the diffraction limit mentionedabove, rather than the seeing limit of ground based observatories.
HubbleLaunched in 1990, the Hubble Space Telescope has taken many of the mostrecognizable space images.
It didn't work too well at first, and so a repair mission had to be sent.Astronauts fixed it.
Fig.35The Orbiting AstronomicalObservatory (OAO) satellites were aseries of four American spaceobservatories launched by NASAbetween 1966 and 1972, whichprovided the first high-qualityobservations of many objects inultraviolet light.
Fig.36The Hubble Space Telescope
Fig.37Hubble before and after
PHY 454 - instruments - J. Hedberg - 2018
updated on 2018-09-27 Page 11
Other improvements1. Active Optics - mirrors that move.2. Adaptive Optics - guide stars
Fig.38The telescope that ateastronomy.
Fig.39Inspecting the mirrors on theJames Webb Space Telescope
Fig.40The primary mirror of NASA'sJames Webb Space Telescope,consisting of 18 hexagonal mirrors,looks like a giant puzzle piece standingin the massive clean room of NASA'sGoddard Space Flight Center inGreenbelt, Maryland.
The idea of adaptive optics has improved observing tremendously. If youcreate an artificial star using a laser, then you should know what is should looklike. Simply adjust your optics in real-time to keep the laser-star looking good!
Fig.41An artificial star
Fig.42Saturn without and withAdaptive Optics
Credit: Heidi B. Hammel and Imke DePater/WMKO Keck