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Chapter 3 Stars: Distances & Magnitudes Nick Devereux 2006 Revised 8/2012

Chapter 3 Stars: Distances & Magnitudes Nick Devereux 2006 Revised 8/2012

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Page 1: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Chapter 3

Stars: Distances & Magnitudes

Nick Devereux 2006 Revised 8/2012

Page 2: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Astrophysical Units & Constants

In addition to the usual list of physical constants – listed inAppendix A (pg A-2), there is another list of astronomicalconstants that we must be familiar with and these are listed in on page A-1.

Nick Devereux 2006

Page 3: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

The Sun as the “yardstick”

Since the distances and masses are so large in astronomy,the basic units of measurement are expressed in terms of theSun.

The Astronomical Unit (AU) is the distance between the Earth andthe Sun,

1 AU = 1.496 x 1011 m

Which is perhaps more familiar to you as 93 million miles.

Nick Devereux 2006

Page 4: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

for larger distances, there is the parsec (pc)

1 pc = 3.086 x 1016 m

The parsec

Nick Devereux 2006

Page 5: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Angular unitsAstronomers can measure the angular extent on the sky forcelestial objects, even if they don’t know how far away theyare, and therefore unable to attribute a linear size.

Radians

360o = 2 radians

So, 1o = 2 radians

or, 1o = radians

Nick Devereux 2006

Page 6: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Angular Units (continued)Arc seconds (‘’) and Arc Minutes (‘)

1‘ = 60 ‘’

1o = 60 ‘ = 3600 ‘’

From previous page… 1o = radians

So, radians = 3600 ‘’

xradians = 1‘’

Or, 1‘’= 4.8 x 10-6 radians and 206265 ‘’ = 1 radian Nick Devereux 2006

Page 7: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Getting back to the pc…..

Nick Devereux 2006

Page 8: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

The pc

(radian) = arc /radius

1‘’/ ‘’/ radian) = 1 AU / 1pc

So, 1 pc = 1 AU x 206265

1 pc = 1.496 x 1011 x 206265 m

Or, 1 pc = 3.086 x 1016 m

Nick Devereux 2006

Page 9: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

In words, a parsec is the distance at which the separation between the Earth and the Sun could be resolved with a medium sized telescope…

Nick Devereux 2006

Page 10: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

What does resolved mean?

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Page 11: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

The Resolving Power of a Telescope

Depends on both the size of the telescope mirror, D,and the wavelength, ,of the light under observation.

(radian) = 1.22 /D

with and D in the same units.

For the Hubble Space Telescope D = 2.4mand = 0.05‘’ @ = 5500 Å .

Nick Devereux 2006

Page 12: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Question: How far away would you have to hold a dime (2cm in diameter) for it to subtend an angle of 1‘’, 0.l‘’ ?

Nick Devereux 2006

Page 13: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Mass

Usually, the masses of stars, galaxies, clusters of galaxiesare given in terms of the mass of the sun,

1 M = 1.99 x 1030 kg

Nick Devereux 2006

Page 14: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Measuring Brightness

Brightness is measured in a variety of ways;

eg. Magnitude, Flux, and Luminosity

Nick Devereux 2006

Page 15: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Luminosity of the Sun

The luminosity of the Sun,

1 L = 3.9 x 1026 W

You may recall that Watts = Joules/sec, so the luminosity of the Sun is a measure of the rate of flow of energy through the surface of a star.

Concept: Think of luminosity as the rate at which a star emits packets (photons) of energy…

Nick Devereux 2006

Page 16: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

FluxThe further you move away from the star, the flux of photons,(measured in units of W/m2) passing through a 1m x 1m area goes down as the reciprocal of the distance squared;

Nick Devereux 2006

Page 17: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Flux (continued)

Quantitatively,

the flux f = L/4D2

Units: W/m2

Nick Devereux 2006

Page 18: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

MagnitudesThe magnitude scale dates back to the Greek astronomer Hipparchus (200 BC).

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Page 19: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Nick Devereux 2006

Page 20: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Definition of Magnitude

The human eye perceives, as linear, what are actually logarithmic differences in brightness.

m = -2.5log f + c

m is the apparent magnitudef is the fluxc is a constant related to the flux of a zero magnitude star

Note the –2.5, the brighter the star (f increases), the more negative the magnitude (m decreases).

Nick Devereux 2006

Page 21: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Differences in magnitudes are equivalent to ratio’s of fluxes

This obviates the need to know the constant c, or, the zero point,of the magnitude scale because;

m1 = -2.5log f1 + cm2 = -2.5log f2 + c

m1 – m2 = 2.5 log f2 / f1

Note the c’s cancelled (c – c = 0)

Also, beware the subscripts are reversed on either side f the equals sign.

Nick Devereux 2006

Page 22: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Question: A binary star system has one star that is 8 times brighter than the other. What is the magnitude difference between the two stars?

Nick Devereux 2006

Page 23: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Absolute Magnitude

We are unable to tell just by looking at the night sky if one staris fainter than another because it is intrinsically fainter (ie. lowerluminosity) or just further away.

To realistically compare stars on an equal basis we introduce the concept of Absolute magnitude (M) which is the magnitude starshave if they are all placed at the same reference distance of 10 pc.

Nick Devereux 2006

Page 24: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

--------------------------------------------------------------------- * (2) d(pc)

----------------------------* (1) 10 pc

f1 = L/410)2 and f2 = L/4 d2

M – absolute magnitude = -2.5log f1 +cm – apparent magnitude = -2.5log f2 +c

Then,

M-m = 2.5log f2 / f1

M-m = 2.5log L 4 10)2 /4 d2 .L

M-m = 2.5log 100/d2 Nick Devereux 2006

Page 25: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Distance ModulusM-m = 5 – 2.5log d2

M-m = 5 – 5log d

So, the absolute magnitude,

M = m + 5 – 5log d

(remember, the distance d must be in pc)

On rearranging,

m - M= 5log d – 5

Where the quantity m – M is known as the distance modulus

Nick Devereux 2006

Page 26: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Trigonometric ParallaxOf course, to calculate the absolute magnitude of a star, we mustknow it’s distance. Distances to nearby stars can be found usingTrigonometric parallax.

Nick Devereux 2006

Page 27: Chapter 3 Stars: Distances & Magnitudes  Nick Devereux 2006 Revised 8/2012

Parallax Angle Question:

Given the definitions for angular units provided earliershow that the parallax angle, measured in arc seconds is equal to the reciprocal of the distance to the star in pc.

So that,

= 1/d

The nearest star Centauri at a distance of 1.3 pc has a parallax angle = 1/1.3 = 0.77’’

. All other stars have even smaller parallaxes. Nick Devereux 2006