BINARIES Read Your Textbook: Foundations of Astronomy –Chapter 10 Homework Problems Chapter 9...

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BINARIES• Read Your Textbook: Foundations of Astronomy

– Chapter 10

• Homework Problems Chapter 9– Review Questions: 1, 4, 5, 7– Review Problems: 1-5– Web Inquiries: 1

• Homework Problems Chapter 10– Review Questions: 1, 2, 4, 6-8– Review Problems: 1-4, 8– Web Inquiries: 2

Binary Center of MassBalance

point

Binary Separation a = rA + rB

Visual

Binary

Star

SpectroscopicBinary

From Doppler Shift

Spectroscopic OrbitThis represents the orbit of the star that is farthest

from the center of mass. Its velocity amplitude is

higher. It is the lower mass star.

Vel

ocit

y

Time

Spectroscopic OrbitThis represents the orbit of the star that is closest

to the center of mass. Its velocity amplitude is

smaller. It is the higher mass star.

Vel

ocit

y

Time

Spectroscopic ParametersCenter of Mass

Low Mass Star Velocity Amplitude

High Mass Star Velocity Amplitude

Vel

ocit

y

Time

InclinationK velocity = amplitude of radial velocity (m/s)

Doppler effect is maximized for an “edge-on” system;

non-existent for a “pole-on” system.

Inclination ~ 90o

Inclination ~ 0o

InclinationK velocity = amplitude of radial velocities

v sin(i)

v = velocity

i = 90 degrees, edge on

i = 0 degrees, pole face

Spectroscopic Parametersvelocity = velocity of Center of Mass (CoM)

K velocity = amplitude of radial velocity (v sin i)

P = period

Mass ratio M2/M1 = K1/K2

Smaller star orbits farther from the CoM,

Larger star is closer from the CoM.

Smaller star has large K velocity.

Spectroscopic Orbit

Center of Mass Velocity?

Spectroscopic Orbit

Orbital Period?

Spectroscopic Orbit

Spectroscopic Orbit

K velocities?

Spectroscopic Orbit

K2 = 115 - 40 = 75

Spectroscopic Orbit

K1 = 65 - 40 = 25

Spectroscopic OrbitK2/K1= M1/M2 = 75/25 = 3

One Star is 3 times more massive than the other.

Eclipsing Binary

Light Intensity variations are observed

because of blocking of light by each of the

stars in the system if inclination is large enough.

Systems are edge-on or nearly edge-on as seen from

earth. (i.e. inclinations are ~ 90 degrees)

Algol ( Perseus)Light Curve

Light Intensity

versus

Time

Eclipsing Binary Light Curve

AB

Eclipsing Binary Light Curve

AB

LA + LB

LA + LB

LB + f LA

LA Only

Eclipsing Binary Light Curve

AB

LA + LB

LA + LB

LB + f LA

LA Only

Eclipsing Binary Light Curve

AB

LA + LB

LA + LB

LB + f LA

LA Only

Eclipsing Binary Light Curve

AB

LA + LB

LA + LB

LB + f LA

LA Only

Simple Eclipsing Binary

Unequal Temperature and Size

Star Spots

Light Curve Fit

Light Curve Varieties

Light Curve Contacts

Light Curve Contacts

t1

Time interval (t2 - t1) ~ size of “orange” star

t3 t4t2

Light Curve Contacts

t1

Time interval (t3 - t1) ~ size of “yellow” star

t3 t4t2

Size Determinations 2 RA = (VA+VB ) ( t2 - t1 )

2 RB = (VA+VB ) ( t3 - t1 )

Velocities obtained from spectroscopic orbit.

Contact times obtained from eclipse light curve.

The radii of the stars are then calculated to yield their

size.

Determining Radii

Intrinsic Luminosity L = 4R2T4

Radius obtained from spectroscopic orbit with

eclipse light curve.

Temperature obtained from observations of spectrum.

Fundamental Stellar Parameters• Spectra

– Distance– Temperature– Chemical Composition– Luminosity (if distance is known)– Velocity

• Binaries– Orbital Velocities– Sizes– Masses– Luminosity

Fundamental Stellar Parameters