Stellar Spectroscopy

26
National Schools’ Observatory Stellar Spectroscopy

description

Stellar Spectroscopy. Introduction. Spectroscopy is a branch of science that is concerned with the investigation and measurement of the spectrum of light produced when matter interacts with electromagnetic radiation. - PowerPoint PPT Presentation

Transcript of Stellar Spectroscopy

Page 1: Stellar Spectroscopy

National Schools’ Observatory

Stellar Spectroscopy

Page 2: Stellar Spectroscopy

National Schools’ Observatory

Introduction

Spectroscopy is a branch of science that is concerned with the investigation and measurement of the spectrum of light produced when matter interacts with electromagnetic radiation.

In astronomy, spectroscopy is a very useful tool because telescopes can easily measure the spectra of far away objects, such as stars and galaxies.

The following activity will focus on stellar spectroscopy (the spectra of stars) and how those spectra can be used to classify stars.

Page 3: Stellar Spectroscopy

National Schools’ Observatory

Introduction

The intensity of those different wavelength components is then measured to create a spectra. The spectra can then be investigated in detail to discover useful information about the target. Rainbows are the spectra of our Sun.

The Liverpool Telescope (LT) has its own spectrograph – FRODOspec (Fibre fed Robotic Dual-beam Optical Spectrograph), and the following activity uses real data taken by the LT using FRODOspec.

We measure the spectra of luminous objects by attaching a special instrument to a telescope, known as a spectrograph.

Within the spectrograph, light is passed through a series of prisms and mirrors in order to split the light into its different component wavelengths (its spectrum).

Page 4: Stellar Spectroscopy

National Schools’ Observatory

FRODOspec

The above image shows the inside of FRODOspec during its development.

Light collected by the telescope enters the FRODOspec instrument and is split into two beams: Longer wavelength light is sent

down the ‘red arm’. Shorter wavelength light is sent

down the ‘blue arm’. The light from each arm is then split

as it passes through a prism, and a detector captures the resulting spectrum on a CCD device.

Page 5: Stellar Spectroscopy

National Schools’ Observatory

FRODOspec

The image to the right shows the raw spectrum of the star BD-02-5059. Each of the vertical lines are repeats

(or orders) of the same spectrum.

You can see a line feature (circled red) running across those orders.

In this activity you will be provided with a 2-D spectrum (wavelength versus intensity) that has been extracted from the raw data.

Page 6: Stellar Spectroscopy

National Schools’ Observatory

Types of Spectra

In general, there are two types of spectra that can be easily identified, EMISSION spectra and ABSORPTION spectra.

An example of an emission spectra:

An example of an absorption spectra:

Page 7: Stellar Spectroscopy

National Schools’ Observatory

Emission Spectra

Due to the temperature of the gas, the atoms within it will possess lots of energy, and some of their electrons will occupy excited states around the nucleus.

These electrons will de-excite (loose energy and fall to a lower energy level), with the lost energy being emitted as a photon at a specific wavelength.

Such processes cause bright lines in a spectra – Emission lines.

Emission spectra occur when electromagnetic radiation originates from a cloud of relatively hot (compared to its surroundings) gas.

Page 8: Stellar Spectroscopy

National Schools’ Observatory

Absorption Spectra

Radiation at specific wavelengths from the star interacts with (is absorbed by) atoms in the cold gas, causing their electrons to gain energy and enter excited states.

These electrons quickly de-excite and emit photons at the same wavelengths. However, the direction of the emitted light is random and this leads to the appearance of dark lines (or missing light) in the resulting spectra, corresponding to the wavelengths that were absorbed by the gas. These lines are known as absorption lines.

Astronomers most frequently use absorption spectra to study stars.

Absorption spectra occur when electromagnetic radiation from a background star passes through a relatively cold gas.

Page 9: Stellar Spectroscopy

National Schools’ Observatory

Absorption Spectra

Temperature Rotational velocity Radial velocity (motion of the star towards or away) Density Chemical composition Metallicity (how many heavy elements stars

contain)

With careful analysis of the absorption lines, astronomers can learn many things about as star, including:

Image of the Pleiades Star

ClusterSome astronomers liken the spectrum of a star to a very basic DNA test that allows them to determine what kind of star the light originated from.

Page 10: Stellar Spectroscopy

National Schools’ Observatory

Chemical Composition

Certain elements and molecules preferentially absorb and emit light at different wavelengths.

It is possible to deduce from spectra which elements are causing lines at particular wavelengths, and hence determine the chemical composition of the object being observed.

Analysis of a spectrum of the Sun led to the discovery of Helium, even before it was discovered on Earth!

Above: Emission spectra of different elements.

Page 11: Stellar Spectroscopy

National Schools’ Observatory

Blackbody Radiation

Before investigating real spectra, we need to talk about Blackbody radiation.

All stars are made up of a hot, dense interior and a cooler outer layer, or atmosphere.

The interior of the star causes a continuous spectrum, known as a blackbody spectrum.

If there was no absorption or emission from the surrounding atmosphere, a star’s spectrum would be close to a pure blackbody spectra.

The blackbody curve (see next slide) represents the spread of intensity of the radiation being emitted over all possible frequencies.

A metal glowing red hot in a furnace is an example of blackbody radiation.

The shape of the blackbody spectrum depends on the temperature of the body.

Page 12: Stellar Spectroscopy

National Schools’ Observatory

Blackbody Radiation

Warmer objects have blackbody spectra that peak at shorter wavelengths, whereas cooler objects have blackbody spectra that peak at longer wavelengths.

Page 13: Stellar Spectroscopy

National Schools’ Observatory

Blackbody Radiation

In reality the measured spectra is never a perfectly smooth blackbody (BB) due to absorption and emission features. The dips in the curve (where it

drops below the BB spectra) represent ABSORPTION lines.

The peaks (where it rises above the BB spectra) represent EMISSION lines. An example of a spectra showing absorption and

emission features (Sloan Digital Sky Survey).

Page 14: Stellar Spectroscopy

National Schools’ Observatory

Wien’s Law

In order to classify a star, it is important for an astronomer to know the temperature of that star.

Stars range in temperature from about 2000K to 40,000K. Using Wien’s law, it is possible to calculate the surface temperature, or

‘effective’ temperature, if we know the wavelength its blackbody curve peaks at.

where W is Wien’s constant and = 2.898×10−3 m·K. maxWTeff

As an example, our Sun’s blackbody spectrum peaks at a wavelength of around 500 x 10-9 m, giving an effective temperature of about 5800K.

Page 15: Stellar Spectroscopy

National Schools’ Observatory

The Doppler Effect

One important effect, the Doppler Effect, occurs due to an apparent shift in the wavelength and frequency of a wave due to relative motion between the source and the observer.

For example, we experience the Doppler Effect when an ambulance drives past with its sirens on: As the ambulance (the source) approaches you (the observer), the sound wave is

compressed (bunched up) and the resulting sound is higher pitched (shorter λ) Once the ambulance has passed, the wave is stretched and the pitch sounds lower

(longer λ)

Shorter wavelength

Longer wavelength

Page 16: Stellar Spectroscopy

National Schools’ Observatory

The Doppler Effect

The same effect is observed with light, when a star (the source) is moving towards or away from observers located on the Earth.

We can detect this motion in the spectrum of the star. If the star is moving AWAY from the Earth, the light waves are stretched out and the

whole spectrum experiences a shift towards the red end of the spectrum – a red shift. If the star is moving TOWARDS the Earth, the light waves are bunched up and the

spectrum experiences a shift towards the blue end of the spectrum – a blue shift.

Shorter wavelength

Longer wavelength

Page 17: Stellar Spectroscopy

National Schools’ Observatory

Spectral Lines

If there were no external factors at play, the absorption spectrum of a star would show very thin spectral line features at the exact wavelengths corresponding to amount of energy transferred to the atom when one of its electrons has been excited to a higher energy level.

In reality, there are a number of different factors that act to spread out or blur the spectral lines across a wider range of wavelengths, a process called spectral line broadening.

Page 18: Stellar Spectroscopy

National Schools’ Observatory

Spectral Line Broadening

The images below are of the same absorption line feature, in this case due to hydrogen, as it appears in the spectra of three different stars.Spectral broadening can be caused by a number of different factors, including:

Temperature (Doppler Broadening) Stellar Rotation Pressure

Page 19: Stellar Spectroscopy

National Schools’ Observatory

Doppler (Thermal)Broadening

The Doppler broadening of spectral lines is the major factor is stellar spectra. Atoms in a gas move around at different speeds and in different directions .

This movement can cause light to be Doppler shifted as an atom in motion emits a photon, and because some of the atoms will be moving away from the observer and some moving towards, the overall effect will contain both blue-shift and red-shift components.

In a hot gas, the atoms possess more energy and thus move around more quickly than in a cooler gas. This means that Doppler broadening is more significant in hot stars.

Hot StarCool Star

Page 20: Stellar Spectroscopy

National Schools’ Observatory

Rotational Velocity

Stars are not just static objects as they appear in the night sky.

They are made up of a fluid mass of gas and plasma (hot gas) that rotates around a common axis. The Sun rotates about once every 24.5 days.

When we obtain the spectra of distant stars, however, the light is gathered from across the entire disc of the star and not from just one point.

Page 21: Stellar Spectroscopy

National Schools’ Observatory

Rotational Velocity

This means that some of the distant star is rotating towards us and some away.

The parts rotating TOWARDS the observer are blue-shifted.

The parts rotating AWAY from the observer are red-shifted.

The net effect is that the star’s spectral lines appear to be smeared out, or rotationally broadened.

Page 22: Stellar Spectroscopy

National Schools’ Observatory

Spectral Classification

It is possible to use the absorption spectra of individual stars to classify them into distinct groups.

Astronomers classify them by temperature, into groups “OBAFGKM”, with group O containing the hottest and M containing the coolest.

Note that there is a direct correlation

between temperature and mass.

Page 23: Stellar Spectroscopy

National Schools’ Observatory

Spectral Classification

These groups are further divided into sub-groups numbered from 0 to 9, where 0 is the hottest; for example, B1 is hotter than B3, and F2 is hotter than F9.

The Sun has a surface temperature of 5800K, putting it in the G2 classification.

Page 24: Stellar Spectroscopy

National Schools’ Observatory

Activity

Now you know a little more about stellar spectroscopy, you will soon get the chance to look at some real spectra from the Liverpool Telescope! Your teacher will supply you with an Excel file containing the 2-D spectral data for 9 stars, each under its own separate tab or page of the worksheet. You are required to plot the spectra for each of these stars. Plot the number of counts against the wavelength for each star. You should

produce spectra similar to the one seen below (don’t forget to label your axes appropriately).

The shape of each spectrum will vary due to the spectral class of the star.

The nine spectra cover many of the different classes of stars.

Wavelength (Angstroms)

Intensity

Page 25: Stellar Spectroscopy

National Schools’ Observatory

Activity

Once you have plotted the nine spectra, you can compare them to see how the different stellar classifications vary. Things to look out for are the width and depth of particular spectral lines.

The Hydrogen line at 6563 angstroms (1 Angstrom is 10-10m) is a good absorption line for spotting any differences.

Hotter stars will have a wider absorption lines due to Doppler broadening.

Cooler stars tend to have more erratic spectra than hotter stars.

Some spectral lines will appear in some stars, but not in others.

Wavelength (Angstroms)

Intensity

Make notes of your observations !

Page 26: Stellar Spectroscopy

National Schools’ Observatory

Activity

Once you’ve had a good look at the spectra of the 9 known star types, it’s time to use this knowledge to classify stars of an unknown star type.

Your teacher will now supply you with another Excel file containing the spectra for two stars that you will have to plot and then classify.

Using the information provided in this presentation, and by making comparisons to the spectra you have already plotted, try to classify the mystery stars.

Good luck!

p.s. If you are really stuck, your teacher will have the answer.