Optical telescopes (ch1?)

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AQA A-level physics options - astrophysics. Telescopes; ch1

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18 Terms

1
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What does it mean when a telescope is in normal adjustment?

the focal points of the eyepiece and the objective lenses meet

2
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<p>label the telescope diagram</p>

label the telescope diagram

Lens = objective lens

eyepiece = eyepiece lens

Where rays meet is called the focal point

<p>Lens = objective lens</p><p>eyepiece = eyepiece lens</p><p>Where rays meet is called the focal point</p>
3
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Equation for magnification in normal adjustment (with focal lengths)

M = fo / fe

Where fo is focal length of objective lens and fe is the focal length of the eyepiece lens.

4
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What are the disadvantages of refracting telescopes?

  • large diameter lenses are difficult to manufacture

  • large diameter lenses are heavy and tend to distort under their own weight

  • suffer from chromatic aberration

  • suffer from spherical aberration

  • not easy to maneuver quickly

  • difficult to mount heavy observing equipment and electronics

  • large magnifications require large objective lenses and long focal lengths therefore require big observatories and domes.

5
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What is chromatic aberration?

When light of different colours enter the tube, they all refract at different angles, therefore have different focal points. As the angle of refraction is dependent on wavelength. This causes a distortion in images.

6
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What is spherical aberration?

When the shape of the objective lens is not perfectly spherical, resulting in multiple focal points and image distortion.

7
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Draw a diagram of a Newtonian reflecting telescope

  • The primary mirror is ideally parabolic, eliminating spherical aberration

  • the spherical mirror is flat

<ul><li><p>The primary mirror is ideally parabolic, eliminating spherical aberration</p></li><li><p>the spherical mirror is flat</p></li></ul><p></p>
8
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Draw a diagram of a Cassegrain reflecting telescope

  • primary mirror is ideally parabolic, eliminating spherical aberration

  • the secondary mirror is convex (bends rays towards eyepiece)

<ul><li><p>primary mirror is ideally parabolic, eliminating spherical aberration</p></li><li><p>the secondary mirror is convex (bends rays towards eyepiece) </p></li></ul><p></p>
9
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Advantages of reflecting telescopes

  • large mirrors can be made easily, they are lighter and easier to support than lenses

  • Mirror surfaces can be made nm thick, giving excellent image properties

  • Mirrors only use front surface for reflection

  • No chromatic aberration

  • No spherical aberration if mirrors are parabolic

  • Make lightweight telescopes, allowing for easy maneuverability for fast response to astronomical events

  • smaller segmented mirrors can be used to form a large composite objective mirror

10
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What are the limitations of ground-based telescopes?

  • atmosphere absorbs and scatters light (ozone, O2, CO2, dust)

  • Atmospheric turbulence reduces image quality

  • Light pollution

11
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How does atmospheric turbulence reduce the image quality of a telescope?

Caused by changes in the refractive index of the atmosphere e.g. due to wind. Light is scattered randomly and results in stars appearing to twinkle. If refractive index of the atmosphere is constant, they do not twinkle.

12
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What is an airy disk?

The bright central region in an optical diffraction pattern caused by light entering a circular aperture.

Each point in an image has its own airy disk. So when the airy disks are large, sometimes two separate objects overlap and become indistinguishable.

<p>The bright central region in an optical diffraction pattern caused by light entering a circular aperture.</p><p>Each point in an image has its own airy disk. So when the airy disks are large, sometimes two separate objects overlap and become indistinguishable.</p>
13
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How do airy disks form?

  • Light enters a circular aperture

  • This causes light rays to diffract, resulting in a circular diffraction pattern

  • sinθ = nλ/d where d is the diameter of the telescope, n is the order, λ is the wavelength of light, and theta is the angle between central maximum and order n.θ ≈ λ D

<ul><li><p>Light enters a circular aperture</p></li><li><p>This causes light rays to diffract, resulting in a circular diffraction pattern</p></li><li><p>sin<span>θ = n</span><strong>λ/d </strong>where d is the diameter of the telescope, n is the order, <strong>λ </strong>is the wavelength of light, and theta is the angle between central maximum and order n.θ ≈ λ D</p></li></ul><p></p>
14
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What is the Rayleigh criterion?

θ ≈ λ/D, sinθ can be approximated to θ using the small angle approximation for sine.

when θ is small, size of airy disk is also small.

The critical point is when the central peal of one of the airy disks overlaps with the first minimum of the other airy disk. In that instance, the objects will be barely resolvable.

15
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What does it mean for two objects to be barely resolvable?

When the central peak of one of the airy disks overlaps with the first minimum of the other airy disk. This is part of the Rayleigh criterion.

16
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Equation and definition for angular resolution.

θ = x/L where x is the distance between objects, and L is the distance from the telescope.

Angular resolution = resolving power. When θ is small, the resolution is high.

17
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What is LGP?

Light gathering power, collecting power for optical telescopes.

This is directly proportional to the diameter of the objective element of the telescope squared. The larger the LGP, the brighter the image.

(area, larger area = more light collected)

18
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what is meant by the minimum angular resolution?

The minimum angle an instrument can distinguish between two small objects for a specific wavelength of EM radiation, as determined by the Rayleigh criterion.