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Lecture 11 Understanding Stars - the H-R Diagram

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1 Lecture 11 Understanding Stars - the H-R Diagram
Our Place in the Cosmos Lecture 11 Understanding Stars - the H-R Diagram

2 Understanding Stars We saw in the last lecture that by measuring the brightness, distance (via parallax) and spectrum of a star, we can determine the following physical properties Surface temperature Radius Luminosity Mass (for binary stars) Just knowing these properties does not mean that we understand stars

3 H-R Diagram The Hertzsprung-Russell diagram (H-R diagram for short) enables one to see patterns in the properties of stars It is named after Einar Hertzsprung and Henry Norris Russell, the first astronomers to independently make plots of the luminosity of stars against their temperature or colour, around The H-R diagram allows one to track the birth, life and death of stars

4 The H-R diagram plots luminosity against surface temperature or colour
Hot, blue stars lie to the left, luminous stars lie to the top Both axes are plotted logarithmically so that stars of fixed size lie along diagonal lines as shown Captions

5 H-R Diagram and Size A star near the top-right corner of the H-R diagram is cool but luminous Stefan’s law L =  A T4 tells us that such a star must have a very large surface area A and hence radius r Conversely, a star near the lower-left is hot but dim, so it must be very small The H-R diagram thus also allows one to gauge sizes of stars, increasing from lower-left to upper-right

6 The Main Sequence When one plots the locations of many stars on the H-R diagram, they are not spread all over the plot Most stars lie along a well-defined sequence running from lower-right to upper-left This is called the main sequence On the left of it are the hottest, most luminous stars known as O stars On the right lie the coolest, dimmest stars, known as M stars

7 Hipparcos sample of 16,600 stars Brightest Closest

8 Distance Estimates The Main Sequence is of great practical use in estimating distances to stars too far away to measure a trigonometric parallax We can determine a star’s colour or surface temperature independent of distance via photometry or spectroscopy respectively If it lies on the main sequence than we can read its approximate luminosity off the H-R diagram Comparing apparent brightness with luminosity then yields an estimate of distance This distance estimate is known as photometric parallax or spectroscopic parallax

9 Selection Effects The distribution of stars on the H-R diagram depends strongly on how they are selected The stars very close to the Sun are mostly dimmer and cooler than the Sun The (apparently) brightest stars in the sky are mostly more luminous and hotter than the Sun There are more cool, dim stars in the Galaxy than hot luminous stars, and these dominate the small volume of space near the Sun By selecting stars by apparent brightness rather than distance, we preferentially select the most luminous stars

10 Stellar Mass Stellar mass increases from lower-right to upper-left along main sequence Stars less massive than the Sun are cooler, redder, smaller and dimmer Stars more massive than the Sun are hotter, bluer, larger and more luminous The mass of a star determines its position on the main sequence and its ultimate fate Mass is the primary determining characteristic of any main sequence star

11 More massive main sequence stars are …
more luminous… …larger… …and hotter (Note logarithmic axes)

12 Mass determines location of a star on the main sequence
High-mass stars are hot and luminous Low mass stars are cool and dim

13 Non-Main Sequence Stars
Although the majority of stars lie on the main sequence (MS), some do not Some stars lie above and to the right of the MS - these are bloated, luminous, cool giants with radii 100s-1000s times larger than the Sun In the lower-left of the H-R diagram lie tiny (and hence dim) but very hot stars Before studying these non-MS stars, we will first study a prototypical MS star - the Sun

14 The Structure of the Sun
Being so close, we can study the Sun - a prototypical MS star - in much greater detail than any other star Our understanding of the Sun comes from many decades of careful observation, theory and computer modelling The Sun is a huge ball of hot gas, held in balance by hydrostatic equilibrium Gravity, which unopposed would cause the Sun to collapse, is balanced by pressure The Sun’s surface is thus in equilibrium

15 Hydrostatic Equilibrium
At each point within the Sun the outward force of pressure is balanced by the inward force of gravity The energy radiated from the Sun’s surface balances the energy produced in its interior

16 Hydrostatic Equilibrium
Towards the centre of the Sun, the weight of the material above becomes greater and so the pressure must increase Gases at higher pressure become denser and hotter Thus density and temperature also increase towards the centre of the Sun Energy must also balance to maintain Sun’s luminosity - just enough energy must be produced in the interior to provide the energy radiated away at the surface

17 NB same data plotted twice… logarithmic linear

18 Sun’s Energy Source The only source of energy efficient enough to provide Sun’s luminosity is nuclear fusion Hydrogen nuclei (single protons) are fused together to make helium nuclei (two protons plus two neutrons) - a process known as hydrogen burning or hydrogen fusion All main sequence stars get their energy from hydrogen fusion

19 Hydrogen Fusion According to Einstein’s famous equation E = mc2, mass and energy are equivalent The mass of four hydrogen atoms is times greater than the mass of a single helium atom In hydrogen fusion, the excess mass is converted to energy Fusing 1 gramme of hydrogen into helium releases about 600 billion Joules of energy - enough to boil the water in about 10 swimming pools The Sun converts roughly 600 million tonnes of hydrogen into helium each second, releasing x 1026 Watts [Joules per second]

20 Hydrogen Fusion Why is hydrogen fusion so hard to achieve on Earth?
The reason is that hydrogen nuclei (protons) have a positive electric charge Two like charges experience a force known as electrostatic repulsion, this makes it extremely difficult to get two hydrogen nuclei close enough to bind (a separation of around metres) Extremely high densities and temperatures are required to overcome electrostatic repulsion - conditions that are ordinarily only found in the cores (central regions) of stars In the Sun’s core the density is about 150 times that of water and the temperature is about 15 million K

21 Slow-moving protons are repelled by electrostatic repulsion
The faster they move, the closer together they can get At high enough temperatures protons move fast enough that they may overcome electrostatic repulsion and fuse together

22 Why Hydrogen Fusion? Hydrogen is the most abundant element in the Universe Hydrogen fusion is the most efficient nuclear fusion process, converting a larger fraction of mass to energy than any other process Hydrogen nuclei have a charge of +1 (in units of the electron’s charge) - there is a much greater electrostatic repulsion for other nuclei such as carbon, which contains six protons and so has a nuclear charge of +6 Cannot directly fuse hydrogen into helium - reaction proceeds by a number of chains - the most common of which is the proton-proton chain

23 Proton-Proton Chain Colliding protons first create
deuterium (2H), then helium-3 (3He) and then helium-4 (4He)

24 Testing the Model Starting with just the mass of the Sun and its chemical composition, our Solar model correctly predicts all other observed properties - size, temperature and luminosity For example, if the Sun were larger than it in fact is, it would radiate energy faster However core density would be less and hydrogen fusion would slow down Core would thus cool, pressure decrease and Sun would shrink back to its equilibrium size If Sun were compressed, fusion rate would increase causing Sun to expand back to its equilibrium size

25 Captions

26 Solar Neutrinos Hydrogen fusion as Sun’s energy supply is confirmed by the observation of neutrinos produced as part of the proton-proton chain Neutrinos are incredibly weakly-interacting and can escape from the core of the Sun much faster than photons of radiation A small fraction can however be detected on Earth in underground labs The rate at which neutrinos are detected agrees with the Solar model assuming that neutrinos have some mass, and are not massless as previously thought

27 Summary Most stars lie in a region of the H-R diagram known as the main sequence Main sequence stars, of which the Sun is a proto-typical example, exist in a state of hydrostatic equilibrium Energy is generated in the core of these stars by the fusion of hydrogen nuclei into helium, accompanied by the release of energy and solar neutrinos Energy is transported to the star’s surface and is radiated away

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