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P7 21st Century Science OCR revision

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1 P7 21st Century Science OCR revision

2 P7.1: Naked-eye astronomy

3 Solar System Collection of planets, comets and other objects which ORBIT the sun. The sun is a STAR

4 Year The time it takes the Earth to complete one orbit of the sun.
The Earth takes days to complete one orbit

5 Moon The Moon orbits the Earth.
It takes about 28 days to complete one orbit. The Moon’s orbit is tilted 5 degrees from the plane of the Earth’s orbit period. 27 days (sidereal) 29 days (viewed from Earth)

6 Axis The Earth rotates around an imaginary line called its axis

7 Movement of the sun Sun appears to move across sky from East  West
This is because Earth spins on axis Sun reappears in same place once every 24 hours – solar day Earth spins on its axis (360o) every 23h 56 minutes – sidereal day

8 Why is a sidereal day different to a solar day?
During the sidereal day the Earth moves further along its orbit of the sun. Therefore for the same part of the Earth to face the sun again, the Earth needs to turn for a further 4 minutes. Solar day is 4 minutes longer than a sidereal day

9 Movement of the stars Long-exposure photographs show the stars to be moving in circles around the Pole Star. They are not actually moving, we are simply observing from a spinning Earth. After 23h 56m (SIDE REAL DAY) they will appear to be back in the same place.

10 Constellation A group of stars that form a pattern.
We see different constellations in summer and winter because we have moved around the sun.

11 Movement of the Moon Moon appears to move across sky from EW
Moon takes longer to appear in same part of sky – 24h 49m This is because: As well as Earth’s rotation giving different view of Moon, Moon is also orbiting the Earth Moon orbits from WE so during night the position of the Moon over 28 days appears to slip slowly back through the pattern of stars.

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13 Moving planets We can see some planets with naked eye.
They are also orbiting the sun. This makes their positions appear to change night by night when viewed against the background of fixed stars

14 Retrograde Motion Planets usually appear to move across sky from E  W like the Sun and Moon. Sometimes they appear to go backwards – retrograde motion This is because different planets have different times to orbit the sun so the place we see a planet in the sky depends on where both the planet and the Earth are in their orbits.

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16 Phases of the Moon We can only see the part of the Moon that is lit up by the Sun. As the Moon orbits the Earth we see different parts of the Moon lit up.

17 , What is an eclipse?

18 Solar eclipse – Moon blocks the Sun’s light

19 Lunar eclipse – Moon moves into the Earth’s shadow

20 Shadows Moon and Earth both have shadows
Region of total darkness – umbra Region of partial darkness – penumbra

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22 Why are lunar eclipses more common than solar eclipses?
Because the Earth’s shadow is bigger than the Moon’s shadow

23 Solar eclipses are also rare because the Moon does not often line up exactly with the Sun because the Moon’s orbit is tilted by 5o relative to the plane of the Earth’s orbit.

24 Celestial Sphere Axis from Pole star through axis of Earth
Celestial equator which is extension of Earth’s equator. Astronomers use two angles to describe the positions of astronomical objects. The angles are measured from a reference point in the sky.

25 P7.2: Telescopes and Images

26 Waves and refraction Light travels as waves
Substance that light travels through is a medium Speed of light depends upon medium – as medium changes speed changes Once a vibrating source has made a wave frequency cannot change. So if speed changes, wavelength changes. If a wave changes direction it is called refraction

27 Refraction If a wave changes direction it is called refraction

28 Refraction at lenses Refracting telescopes use convex lenses
Convex lenses are thicker in the middle than the edges If parallel rays enter a convex lens they come to a point called the focus. When rays meet at the focus they have converged.

29 Images in lenses Use these rules to draw ray diagrams
Use arrows to show the direction that light is travelling

30 Images in lenses Use these rules to draw ray diagrams
Use arrows to show the direction that light is travelling A ray through the centre of a lens does not change direction

31 Images in lenses Use these rules to draw ray diagrams
Use arrows to show the direction that light is travelling A ray through the centre of a lens does not change direction A ray parallel to the principal axis passes through the focus

32 Images in lenses Use these rules to draw ray diagrams
Use arrows to show the direction that light is travelling A ray through the centre of a lens does not change direction A ray parallel to the principal axis passes through the focus A ray through the focus emerges parallel to the principal axis principal axis

33 Stars and light rays Stars – very far away
Rays reaching Earth from stars are parallel

34 Stars and light rays Stars – very far away
Rays reaching Earth from stars are parallel Convex lens refracts rays from star through a single point Point is the image of the star.

35 Inverted images Objects in the Solar system are closer than stars.
Light rays from different parts of the object arrive at a lens at different angles Rays from top of object go to bottom of lens and vice versa. This means the image is inverted

36 Focal length and lens power
Focal length – distance from lens to image

37 Focal length and lens power
Focal length – distance from lens to image A fat convex lens has a shorter focal length than a thin lens – fat lens is more powerful

38 Measuring the power of a lens
Units = dioptres Power (dioptres) = 1 / focal length (metres-1)

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40 What’s inside a telescope?
Objective lens (long focal length = low power) Forms image inside telescope Eyepiece lens (short focal length = high power) Magnifies image formed by objective lens Distance between lenses = sum of 2 focal lengths

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42 Why do we use telescopes?
Magnification enables you to see detail you cannot see with the naked eye. They have a greater aperture so they collect more light. This enables you to see dimmer stars than with the naked eye.

43 Magnification The angles between stars appear bigger with a telescope than the naked eye. This is the angular magnification of the telescope. Magnification = focal length of objective lens focal length of eyepiece lens

44 Magnification Example problem Calculate the magnification of a telescope with an objective of focal length 1200 mm using two different eyepieces with focal lengths of: (a) 25 mm   (b) 10 mm

45 Example problem Calculate the magnification of a telescope with an objective of focal length 1200 mm using two different eyepieces with focal lengths of: (a) 25 mm (b) 10 mm (a) Magnification = 1200/25 = 48x (b) Magnification = 1200/10 = 120x

46 Reflecting telescopes
Most telescopes use a concave mirror rather than a lens as the objective. This brings parallel light to a focus. An eyepiece lens then magnifies the image from the mirror

47 Advantages of reflecting telescopes
Easier to make a big mirror than a big lens Hard to make a glass lens with no imperfections Big convex lenses are fat in the middle, glass absorbs light on the way through the lens, so faint objects look even fainter. X 

48 Advantages of reflecting telescopes
Easier to make a big mirror than a big lens Hard to make a glass lens with no imperfections Big convex lenses are fat in the middle, glass absorbs light on the way through the lens, so faint objects look even fainter. Mirrors reflect all colours the same, lenses refract blue light more than red distorting the image.

49 Dispersion White light = mixture of colours
Violet light = higher frequency & shorter wavelength than red light Violet light slows down more in glass so is refracted more In lenses and prisms, refraction splits white light into colours = dispersion

50 Dispersion at a diffraction grating
Dispersion also occurs at a diffraction grating (narrow parallel lines on a sheet of glass). When white light shines on the grating, different colours emerge at different angles. This forms spectra. Astronomers view stars through spectrometers containing prisms or gratings. These show the frequencies of light emitted by the star.

51 Diffraction Diffraction is when waves go through a gap, bend and spread out. The effect is greatest when the size of the gap is similar to or smaller than the wavelength of the waves.

52 Diffraction and telescopes
The light-gathering area of a telescope’s objective lens or mirror is its aperture If diffraction occurs at the aperture, the image will be blurred. Optical telescopes have apertures much bigger than the wavelength of light to reduce diffraction and form sharp images. Radio waves have long wavelengths. A telescope that detects radio waves from distant objects needs a very big aperture.

53 These pictures show images with a 10 meter telescope and a 100 meter telescope.

54 P7.3: Mapping the Universe

55 Light year Distance light travels in one year
After the sun, the nearest stars are about 4 light years away We see light that left those stars 4 years ago Some galaxies are millions of light years away

56 Parallax As the Earth orbits the Sun, the closest starts appear to change positions relative to the very distinct ‘fixed stars’. This effect is called parallax The stars have not actually moved It is the Earth that has moved.

57 Parallax angle HALF the angle the star has apparently moved in 6 months (as we travel from one side of the Sun to the other). Parallax angles are tiny. They are measured in seconds of arc. 1 second of arc = 1/3600 of a degree The smaller the parallax angle, the further away the star. . Distance to star = 1 / parallax angle (in seconds of arc) (parsecs)

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59 Parsecs (pc) A parsec (pc) is the distance to a star whose parallax angle is 1 second of arc. A parsec is similar in magnitude (size) to a light-year Distances between stars within a galaxy are usually a few parsecs Distances between galaxies are measured in megaparsecs (Mpc)

60 Distances between stars within a galaxy are usually a few parsecs
Distances between galaxies are measured in megaparsecs (Mpc)

61 Star luminosity HOTTER and BIGGER = more energy radiated per second
Luminosity = Amount of radiation emitted by a star every second Luminosity depends on: size of the star temperature of the star HOTTER and BIGGER = more energy radiated per second

62 Luminosity variables – size of star
For stars with the same surface temperature the bigger the star the more energy it gives out. A star with double the radius of another one will have an area four times as great and so have a luminosity four times greater than the first star R2 Double the radius R Radius x2 Area x4 Luminosity

63 Luminosity variables – temp of star Double the temperature
For stars of the same size the hotter the star the more energy it gives out. A star with a temperature of double another one will have a luminosity sixteen times greater. T2 Double the temperature T Temperature x2 Luminosity x16

64 Observed intensity How bright a star appears when seen from Earth
Brightness depends on: luminosity of the star distance of the star from the Earth

65 Double the distance from earth
Brightness For two stars of the same luminosity with one star double the distance of the other from the Earth the closer star will look four times brighter. D2 D Double the distance from earth Distance x2 Luminosity x ¼

66 Light spreads out, so the more distant a source is the less bright it appears.

67 Luminosity, brightness and magnitudes
For stars which give out the same amount of light Brightness on Earth as Distance from Earth

68 Cepheid variable stars
Star whose brightness changes with time Variation in brightness thought to be because the star expands and contracts in size (by 30%) causing a variation in temp and luminosity.

69 Calculating the distance to a Cepheid variable star
Measure the period Use the period to work out the luminosity

70 Calculating the distance to a Cepheid variable star
Measure the period – 5 days Use the period to work out the luminosity Measure the observed brightness Compare the observed brightness with the luminosity to work out the distance The period–luminosity relation for Cepheid variables

71 Observing nebulae and galaxies
We know from telescope observations that our galaxy (Milky Way) is made up of millions of stars. The sun is one of the stars in our galaxy In the 1920s astronomers were puzzled by fuzzy patches of light seen through telescopes. They called these fuzzy patches nebulae. Nebulae have different shapes including spirals

72 Shapeley vs. Curtis Curtis Shapeley
Thought Milky Way was entire universe Thought nebulae were clouds of gas within Milky Way Thought spiral nebulae were huge distant clusters of stars – other galaxies outside the Milky Way

73 Shapeley vs. Curtis Neither astronomer had enough evidence to win the argument Later HUBBLE found a Cepheid variable in a spiral nebula, Andromeda. Hubble measured the distance from Earth  star. It was further than any star in the Milky Way galaxy He concluded that the star was in a separate galaxy Cepheid variable stars have been used to show that most spiral nebulae are distant galaxies, of which there are billions in the Universe.

74 The amazing and expanding Universe!
Astronomers study absorption spectra from distant galaxies Compared to spectra from nearby stars, the black absorption lines for distant galaxies are shifted towards the red end of the spectrum. This is REDSHIFT Redshift shows us that galaxies are moving away from us.

75 (you can use either set of units)
Speed of recession Redshift shows us that galaxies are moving away from us. The speed of recession of a galaxy is the speed at which it is moving away from us. This can be found from the redshift of the galaxy. (you can use either set of units)

76 Hubble, Cepheid Variables and Recession
Hubble measured the distance to Cepheid variable stars in several galaxies. He found the further away a galaxy is, the greater its speed of recession.

77 Hubble’s constant Since Hubble, many astronomers have gathered data from Cepheid variable stars in different galaxies. These data have given better values of the Hubble constant. The fact that galaxies are moving away from us suggests that the Universe began with a big bang about 14 thousand million years ago. Distant galaxies seem to be moving away faster than nearby galaxies, hence scientists conclude that space itself is expanding.

78 P7.4: The Sun, the stars and their surroundings

79 Star Spectra and Temperature
Hot objects (including stars) emit energy across all wavelengths of the EM radiation spectrum Different stars emit different amounts of radiation and different frequencies depending on their temperature.

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81 INCREASING TEMPERATURE

82 Spectrometer Peak frequency = Higher temperature
Used by astronomers to: Measure radiation emitted at each frequency Identify the peak frequency of a star The peak frequency gives an accurate value for the temperature of a star. Peak frequency = Higher temperature

83 Identifying elements in stars
Astronomers use spectra from stars to identify their elements. The surface of the Sun emits white light. As the light travels through the Sun’s atmosphere, atoms in this atmosphere absorb light of certain frequencies. The light that travels on has these frequencies missing. When the light is spread into a spectrum, there are dark lines across it. This is the absorption spectrum of the sun

84 Identifying elements in stars
Each element produces a unique pattern of lines in its absorption spectrum Astronomers identify the elements in stars by comparing star absorption spectra to those of elements in the lab

85 How do gases behave? Stars are balls of hot gases
To understand stars, you need to understand gases The particles of a gas move very quickly in random directions When they hit the sides of a container they exert a force as they change direction  this causes gas pressure

86 Pressure and volume If you decrease the volume of the container, the particles hit the sides more often and the pressure increases

87 pressure x volume = constant
Pressure and volume Volume and pressure are inversely proportional For a fixed mass of gas at constant temp as volume decreases pressure increases pressure x volume = constant

88 Pressure and temperature
The hotter the gas, the more energy the particles have and the faster they move The faster the particles move, the harder and more often they hit the sides of the container.

89 Pressure and temperature
Temperature and pressure are directly proportional For a fixed mass of gas at constant volume as temperature (K) increases pressure increases pressure / temperature = constant

90 Cooling a gas As a gas cools, the particles lose energy & they move more slowly At the lowest temperatures particles stop moving and therefore would never hit the sides of the container. Lowest theoretical temp = absolute zero (-273oC) X

91 Kelvin Scale Starts at the lowest theoretical temp = absolute zero (-273oC) Zero on the Kelvin scale is oC = absolute zero

92 Volume and temperature
If you decrease the temperature of a gas at constant pressure, the volume decreases. At absolute zero, the volume would theoretically be zero For a fixed mass of gas at a fixed pressure: As temp increases, vol increases Volume is directly proportional to temp (K) volume = constant temperature

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94 Inside stars

95 Protostars Gravity compresses a cloud of H and He gas
The gas particles get closer and closer The volume of the gas cloud decreases As they get closer they move faster Temperature and pressure increase This mass of gas is called a protostar

96 Protostars and Nuclear Fusion
When H nuclei get close enough they form He nuclei – nuclear fusion This process releases energy. Protostar star when fusion begins Nuclear fusion happens in all stars including our Sun

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98 Protostar formation

99 Nuclear fusion in the Sun
0 1 + e+ (positron)

100 Nuclear fusion in the Sun
The product of the previous reaction may then fuse with another hydrogen nucleus to form an isotope of helium

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102 Positrons Like an electron, but with a positive charge
Emitted in some nuclear reactions to conserve charge

103 (speed of light in a vacuum)2
Nuclear equations You must balance: Mass (top number) Charge (lower numbers) In fusion reactions the total mass of product particles is slightly less than the total mass of reactant particles. The mass that is lost has been released as energy You can use Einstein’s equation to calculate energy released in nuclear fusion / fission reactions Energy released = mass lost x (speed of light in a vacuum)2

104 Inside stars

105 Stars which fuse H to form He are main-sequence stars (e.g. the sun)

106 Photosphere ~ surface of star
Core Radiative zone Convective zone Photosphere ~ surface of star

107 Temperature and density are highest. Most nuclear fusion happens here
Energy is transported outwards from the core by radiation Convection currents flow here, carrying heat energy to the photosphere Energy is radiated into space from here

108 Inside stars

109 Red giants and supergiant stars
In main sequence stars, H nuclei fuse to form He. Eventually the H runs out The pressure decreases The core collapses Hydrogen containing outer layers of the star fall inwards New fusion reactions happen in the core These reactions make the outer layers of the star expand The photosphere cools and its colour changes from yellow  red A red giant / supergiant has formed

110 Red giants and supergiant stars
While the outer layers of a red giant / supergiant expand, its core gets smaller It becomes hot enough for He nuclei to fuse together to form heavier nuclei The more massive the star, the hotter the core, the heavier the nuclei it can produce by fusion Red giants – fusion reactions produce nuclei of carbon, then nitrogen and oxygen Supergiants (core pressure and temp higher) – fusion reactions produce elements with nuclei as heavy as iron!!

111 Inside stars

112 White dwarf stars The Sun has a relatively low mass
When it becomes a red giant it will not be compressed further once its He has been used up The star will shrink to become a white dwarf star There is no fusion in a white dwarf. It will gradually cool and fade

113 Supernova When the core of a supergiant is mainly iron, it explodes - this is a supernova It is so hot that fusion reactions produce atoms of elements as heavy as uranium

114 After a supernova explosion, a dense core remains.

115 After a supernova explosion, a dense core remains.
Smaller core – neutron star Bigger core – black hole (so much mass concentrated into a tiny space that even light cannot escape from it)

116 Clouds of dust and gas blown outwards by a supernova may eventually form new protostars

117 Hertzsprung-Russell diagram
H-R diagram plots luminosity against temperature For main sequence stars there is a correlation: the hotter the star, the more radiation emitted and so the greater its luminosity

118 Hertzsprung-Russell diagram
H-R diagram plots luminosity against temperature For main sequence stars there is a correlation: the hotter the star, the more radiation emitted and so the greater its luminosity

119 Hertzsprung-Russell diagram
H-R diagram plots luminosity against temperature For main sequence stars there is a correlation: the hotter the star, the more radiation emitted and so the greater its luminosity Increasing luminosity Increasing temperature HOT COOL

120 Hertzsprung-Russell diagram
H-R diagram plots luminosity against temperature For main sequence stars there is a correlation: the hotter the star, the more radiation emitted and so the greater its luminosity You may be asked to identify regions of the H-R in which different types of star are located

121 Exoplanets Astronomers have found evidence of planets orbiting nearby stars. These are exoplanets Some may have the right conditions for life Because of this scientists think there may be life elsewhere in the Universe No evidence of ET life has yet been discovered X

122 P7.5: The astronomy community

123 Choosing your observatory site
Astronomers use huge telescopes to collect weak radiation from faint or very distant sources. Major optical and infrared telescopes on Earth are in: Chile Hawaii Australia Canary Islands

124 Choosing your observatory site
When choosing a site, astronomers consider a number of factors If you have a question in the exam about evaluating telescope sites Compare the advantages and disadvantages of each site State with reasons which site you believe to be best

125 Choosing your observatory site
When choosing a site, astronomers consider a number of factors Factor Solution Atmosphere reflects light This distorts images Choose a high altitude location (e.g. a mountain) to reduce this problem The Sphinx Observatory in the Swiss Alps

126 Choosing your observatory site
When choosing a site, astronomers consider a number of factors Factor Solution Atmosphere reflects light This distorts images Choose a high altitude location (e.g. a mountain) to reduce this problem The Sphinx Observatory in the Swiss Alps

127 Choosing your observatory site
When choosing a site, astronomers consider a number of factors Factor Solution Light is refracted more if the air is damp or polluted Locate your telescope in an area with dry, clean air for higher-quality images Clear skies, dry air and low pollution make Arizona a hotspot for astronomy.

128 Choosing your observatory site
When choosing a site, astronomers consider a number of factors Factor Solution Light is refracted more if the air is damp or polluted Locate your telescope in an area with dry, clean air for higher-quality images Clear skies, dry air and low pollution make Arizona a hotspot for astronomy.

129 Choosing your observatory site
When choosing a site, astronomers consider a number of factors Factor Solution Astronomical observation cannot be made in cloudy conditions Choose an area with frequent cloudless nights Clear skies, dry air and low pollution make Arizona a hotspot for astronomy.

130 Choosing your observatory site
When choosing a site, astronomers consider a number of factors Factor Solution Astronomical observation cannot be made in cloudy conditions Choose an area with frequent cloudless nights Clear skies, dry air and low pollution make Arizona a hotspot for astronomy.

131 Choosing your observatory site
When choosing a site, astronomers consider a number of factors Factor Solution Cities cause light pollution Choose an area far from cities Clear skies, dry air and low pollution make Arizona a hotspot for astronomy.

132 Choosing your observatory site
When choosing a site, astronomers consider a number of factors Factor Solution Cities cause light pollution Choose an area far from cities Clear skies, dry air and low pollution make Arizona a hotspot for astronomy.

133 Choosing your observatory site
When choosing a site, astronomers consider a number of factors Other factors: Cost (inc. travel to and from telescope for supplies and workers) Environmental impact near the observatory Impact on local people Working conditions for employees

134 Computer controlled telescopes
Allows astronomers to use a telescope thousands of miles away Images are recorded digitally and sent electronically to computers Computers can then be used to analyse images and improve their quality (e.g. adding colour) Observations can then be shared with other astronomers

135 Why put telescopes in space???
Telescopes on Earth are affected by: Atmosphere (which absorbs most IR, UV, X-ray and gamma radiation) Atmospheric refraction (distorts images and makes stars ‘twinkle’) Light pollution Bad weather

136 Why put telescopes in space???
Telescopes on Earth are affected by: Atmosphere (which absorbs most IR, UV, X-ray and gamma radiation) Atmospheric refraction (distorts images and makes stars ‘twinkle’) Light pollution Bad weather All of these problems are overcome by putting a telescope in space The Hubble Space Telescope has a better resolution than any telescope on Earth

137 Problems with telescopes in space???
High cost of setting up High cost of on-going maintenance and repairing a telescope in space Uncertainties of future funding

138 International collaboration
Allows the cost of a major telescope to be shared Allows expertise to be pooled Exam tip: Know two examples showing how international co-operation is essential for progress in astronomy

139 International collaboration – European Southern Observatory (ESO)
Involves 14 European countries + Brazil Consists of several telescopes in Chile Chile provides the base and the office staff 1000+ astronomers from all over the world use the facility each year

140 International collaboration – Gran Telescopio Canarias
In the Canary Islands At the top of a high volcanic peak Funded mainly by Spain, with contributions from Mexico and the USA Planning involved people from 100 companies


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