Astronomical distances The SI unit for length, the metre, is a very small unit to measure astronomical distances. There units usually used is astronomy:

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Presentation transcript:

Astronomical distances The SI unit for length, the metre, is a very small unit to measure astronomical distances. There units usually used is astronomy:  The Astronomical Unit (AU) – this is the average distance between the Earth and the Sun. This unit is more used within the Solar System. The SI unit for length, the metre, is a very small unit to measure astronomical distances. There units usually used is astronomy:  The Astronomical Unit (AU) – this is the average distance between the Earth and the Sun. This unit is more used within the Solar System. 1 AU = km or 1 AU = 1.5x10 11 m

Astronomical distances  The light year (ly) – this is the distance travelled by the light in one year. 1 ly = 9.46x10 15 m c = 3x10 8 m/s t = 1 year = x 24 x 60 x 60= 3.16 x 10 7 s Speed =Distance / Time Distance = Speed x Time = 3x10 8 x 3.16 x 10 7 = 9.46 x m

Astronomical distances  The parsec (pc) – this is the distance at which 1 AU subtends an angle of 1 arcsencond. 1 pc = 3.086x10 16 m or 1 pc = 3.26 ly “Parsec” is short for parallax arcsecond

1 parsec = X metres  Nearest Star 1.3 pc (206,000 times further than the Earth is from the Sun)

Parallax Angle star/ball appears to shift “Baseline” Distance to star/ball Where star/ball appears relative to background Bjork’s EyesSpace

Parallax, more accurately motion parallax, is the change of angular position of two observations of a single object relative to each other as seen by an observer, caused by the motion of the observer. Simply put, it is the apparent shift of an object against the background that is caused by a change in the observer's position. Parallax, more accurately motion parallax, is the change of angular position of two observations of a single object relative to each other as seen by an observer, caused by the motion of the observer. Simply put, it is the apparent shift of an object against the background that is caused by a change in the observer's position. Parallax

Baseline – R (Earth’s orbit) Distance to Star - d Parallax - p (Angle) We know how big the Earth’s orbit is, we measure the shift (parallax), and then we get the distance… Parallax

For very small angles tan p ≈ p (angles in radians) In conventional units it means that

Parallax

 360 degrees (360 o ) in a circle  60 arcminutes (60’) in a degree  60 arcseconds (60”) in an arcminute Angular sizes

The farther away an object gets, the smaller its shift. Eventually, the shift is too small to see. Parallax has its limits

Another thing we can figure out about stars is their colors… We’ve figured out brightness, but stars don’t put out an equal amount of all light… …some put out more blue light, while others put out more red light!

Usually, what we know is how bright the star looks to us here on Earth… We call this its Apparent Magnitude “What you see is what you get…”

The Magnitude Scale  Magnitudes are a way of assigning a number to a star so we know how bright it is  Similar to how the Richter scale assigns a number to the strength of an earthquake  Magnitudes are a way of assigning a number to a star so we know how bright it is  Similar to how the Richter scale assigns a number to the strength of an earthquake This is the “8.9” earthquake off of Sumatra Betelgeuse and Rigel, stars in Orion with apparent magnitudes 0.3 and 0.9

The historical magnitude scale…  Greeks ordered the stars in the sky from brightest to faintest… …so brighter stars have smaller magnitudes.  Greeks ordered the stars in the sky from brightest to faintest… …so brighter stars have smaller magnitudes. MagnitudeDescription 1stThe 20 brightest stars 2ndstars less bright than the 20 brightest 3rdand so on... 4thgetting dimmer each time 5thand more in each group, until 6ththe dimmest stars (depending on your eyesight)

Later, astronomers quantified this system.  Because stars have such a wide range in brightness, magnitudes are on a “log scale”  Every one magnitude corresponds to a factor of 2.5 change in brightness  Every 5 magnitudes is a factor of 100 change in brightness (because (2.5) 5 = 2.5 x 2.5 x 2.5 x 2.5 x 2.5 = 100)  Because stars have such a wide range in brightness, magnitudes are on a “log scale”  Every one magnitude corresponds to a factor of 2.5 change in brightness  Every 5 magnitudes is a factor of 100 change in brightness (because (2.5) 5 = 2.5 x 2.5 x 2.5 x 2.5 x 2.5 = 100)

Brighter = Smaller magnitudes Fainter = Bigger magnitudes  Magnitudes can even be negative for really bright stuff! ObjectApparent Magnitude The Sun-26.8 Full Moon-12.6 Venus (at brightest)-4.4 Sirius (brightest star)-1.5 Faintest naked eye stars6 to 7 Faintest star visible from Earth telescopes ~25

However: knowing how bright a star looks doesn’t really tell us anything about the star itself! We’d really like to know things that are intrinsic properties of the star like: Luminosity (energy output) and Temperature

…we need to know its distance! In order to get from how bright something looks… to how much energy it’s putting out…

The whole point of knowing the distance using the parallax method is to figure out luminosity… It is often helpful to put luminosity on the magnitude scale… Absolute Magnitude: The magnitude an object would have if we put it 10 parsecs away from Earth Once we have both brightness and distance, we can do that!

Absolute Magnitude (M)  The Sun is in apparent magnitude, but would be 4.4 if we moved it far away  Aldebaran is farther than 10pc, so it’s absolute magnitude is brighter than its apparent magnitude  The Sun is in apparent magnitude, but would be 4.4 if we moved it far away  Aldebaran is farther than 10pc, so it’s absolute magnitude is brighter than its apparent magnitude Remember magnitude scale is “backwards” removes the effect of distance and puts stars on a common scale

Absolute Magnitude (M) Knowing the apparent magnitude (m) and the distance in pc (d) of a star its absolute magnitude (M) can be found using the following equation: Example: Find the absolute magnitude of the Sun. The apparent magnitude is The distance of the Sun from the Earth is 1 AU = 4.9x10 -6 pc Therefore, M= – 5*log (4.9x10 -6 ) + 5 = = +4.8

So we have three ways of talking about brightness:  Apparent Magnitude - How bright a star looks from Earth  Luminosity - How much energy a star puts out per second  Absolute Magnitude - How bright a star would look if it was 10 parsecs away  Apparent Magnitude - How bright a star looks from Earth  Luminosity - How much energy a star puts out per second  Absolute Magnitude - How bright a star would look if it was 10 parsecs away

Spectroscopic parallax  Spectroscopic parallax is an astronomical method for measuring the distances to stars. Despite its name, it does not rely on the apparent change in the position of the star.  This technique can be applied to any main sequence star for which a spectrum can be recorded.  Spectroscopic parallax is an astronomical method for measuring the distances to stars. Despite its name, it does not rely on the apparent change in the position of the star.  This technique can be applied to any main sequence star for which a spectrum can be recorded.

Spectroscopic parallax The Luminosity of a star can be found using an absorption spectrum.  Using its spectrum a star can be placed in a spectral class.  Also the star’s surface temperature can be determined from its spectrum (Wien’s law)  Using the H-R diagram and knowing both temperature and spectral class of the star, its luminosity can be found.