41
ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

  • View
    217

  • Download
    1

Embed Size (px)

Citation preview

Page 1: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

ASTR100 (Spring 2008) Introduction to AstronomyProperties of Stars

Prof. D.C. Richardson

Sections 0101-0106

Page 2: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106
Page 3: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

How do we measure stellar luminosities?

Page 4: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

The brightness of a star depends on both distance and luminosity.

Page 5: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Luminosity:

Amount of power a star radiates.

(Energy per second, or Watts.)

Apparent brightness:

Amount of starlight that reaches Earth.

(Energy per second per square meter.)

Page 6: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Thought Question

These two stars have about the same luminosity. Which one appears brighter to us?

A. Alpha Centauri.B. The Sun.

Page 7: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Thought Question

These two stars have about the same luminosity. Which one appears brighter to us?

A. Alpha Centauri.B. The Sun.

Page 8: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Luminosity passing through each sphere is the same.

Area of sphere:

4 (radius)2

Divide luminosity by area to get brightness.

Page 9: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

The relationship between apparent brightness and luminosity depends on distance…

We can determine a star’s luminosity if we can measure its distance and apparent brightness…

Measuring Luminosity

brightness =luminosity

4π (distance)2

luminosity = 4π (distance)2 × (brightness)

Page 10: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Thought Question

How would the apparent brightness of Alpha Centauri change if it were three times farther away?

A. It would be only 1/3 as bright.B. It would be only 1/6 as bright.C. It would be only 1/9 as bright.D. It would be three times

brighter.

Page 11: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Thought Question

How would the apparent brightness of Alpha Centauri change if it were three times farther away?

A. It would be only 1/3 as bright.B. It would be only 1/6 as bright.C. It would be only 1/9 as bright.D. It would be three times

brighter.

Page 12: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

So how far away are these stars?

Page 13: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Parallaxis the apparent shift in position of a nearby object against a background of more distant objects.

Page 14: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Parallax is measured by comparing snapshots taken at different times and measuring the shift in angle to the star.

Page 15: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Apparent positions of nearest stars shift by about an arcsecond as Earth orbits the Sun.

Page 16: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

The farther the distance, the smaller the angle.

Page 17: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Parallax and Distance

p = parallax angle

d (in parsecs) = 1

p (in arcseconds)

d (in light-years) = 3.26 ×1

p (in arcseconds)

Page 18: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Most luminous stars:

106 LSun.

Least luminous stars:

10-4 LSun.

(LSun is the luminosity of the Sun.)

Page 19: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

The Magnitude Scale

m = apparent magnitude M = absolute magnitude

apparent brightness of Star 1apparent brightness of Star 2

=(1001/5)m1−m2

luminosity of Star 1luminosity of Star 2

=(1001/5)M1−M2

Page 20: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

How do we measure stellar temperatures?

Page 21: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Recall: every object emits thermal radiation with a spectrum that depends on its temperature.

Page 22: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

An object of fixed size grows more luminous as its temperature rises.

Relationship Between Temperature and Luminosity

Page 23: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Properties of Thermal Radiation

1. Hotter objects emit more light per unit area at all wavelengths (more luminous).

2. Hotter objects emit photons with a higher average energy (bluer).

Page 24: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Hottest stars:

50,000 K.

Coolest stars:

3,000 K.

(Sun’s surface is 5,800 K.)

Page 25: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Solid

Molecules

Neutral Gas

IonizedGas(Plasma)

Level of ionization also reveals star’s temperature.

10 K

102 K

103 K

104 K

105 K

106 K

Page 26: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Absorption lines in a star’s spectrum tell us its ionization level.

Page 27: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Lines in a star’s spectrum correspond to a spectral type that reveals its temperature.

(Hottest) O B A F G K M (Coolest)

Fewer lines

More lines

Page 28: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

(Hottest) O B A F G K M (Coolest)

Remembering Spectral Types

“Oh Boy An F Grade Kills Me…”

Also subdivide each type:

e.g., (hottest) A0, A1, …, A9 (coolest).

The Sun is type G2.

Page 29: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Thought Question

Which of the stars below is hottest?

A. M starB. F starC. A starD. K star

Page 30: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Thought Question

Which of the stars below is hottest?

A. M starB. F starC. A starD. K star

Page 31: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Pioneers of Stellar Classification

Annie Jump Cannon and the “calculators” at Harvard laid the foundation of modern stellar classification.

Page 32: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

How do we measure stellar masses?

Page 33: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

The orbit of a binary star system depends on strength of gravity.

Page 34: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Types of Binary Star Systems

Visual binary. Eclipsing binary. Spectroscopic binary.

About half of all stars are in binary systems.

Page 35: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Visual Binary

We can observe the orbital motions of these stars directly.

Page 36: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Eclipsing Binary

We can measure periodic eclipses.

Page 37: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Spectroscopic Binary

We can measure Doppler shifts.

Page 38: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Isaac Newton

We measure mass using gravity.

Direct mass measurements are possible only for stars in binary star systems.

p = period

a = average separation

p2 = a3 4π2

G (M1 + M2)

Page 39: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

r M

v

Need 2 out of 3 observables to measure mass…

1. Orbital period (p).2. Orbital separation (a or r =

radius).3. Orbital speed (v).

4. For circular orbits, v = 2r / p.

Page 40: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Most massive stars:

100 MSun.

Least massive stars:

0.08 MSun.

(MSun is the mass of the Sun.)

Page 41: ASTR100 (Spring 2008) Introduction to Astronomy Properties of Stars Prof. D.C. Richardson Sections 0101-0106

Summary

We have discussed 5 ways of determining stellar properties:1. Distance – use stellar parallax.2. Luminosity – use distance and apparent

brightness (inverse square law).3. Temperature – use color (thermal

radiation law; red = cool, blue = hot).4. Spectral type (OBAFGKM) – use

absorption spectrum (ionization level).5. Mass – use binary stars.

Visual, eclipsing, and/or spectroscopic binaries.